# Negative resistance

(Redirected from Negative differential resistance)
Fluorescent lamp, a device with negative differential resistance.[1][2] In operation, an increase in current through the fluorescent tube causes a drop in voltage across it. If the tube were connected directly to the power line, the falling tube voltage would cause more and more current to flow, until it destroyed itself.[1][3] To prevent this, fluorescent tubes are connected to the power line through a ballast. The ballast adds positive impedance (AC resistance) to the circuit to counteract the negative resistance of the tube, limiting the current.[1]

In electronics, negative resistance (NR) also called negative conductance[4] is a property of some electrical circuits and devices in which an increase in voltage across the device's terminals results in a decrease in electric current through it.[5][6][7] This is in contrast to an ordinary resistor in which an increase of applied voltage causes a proportional increase in current due to Ohm's law, resulting in a positive resistance.[8] While a positive resistance consumes power from current passing through it, a negative resistance produces power.[9] Under certain conditions it can increase the power of an electrical signal, amplifying it.[3][10][11]

Negative resistance is an uncommon property which occurs in a few nonlinear electronic components. In a nonlinear device, two types of resistance can be defined: static or absolute resistance, the ratio of voltage to current $\scriptstyle v/i\,$, and differential resistance, the ratio of a change in voltage to the resulting change in current $\scriptstyle \Delta v/\Delta i$. The term negative resistance refers to negative differential resistance (NDR), $\scriptstyle \Delta v/\Delta i\;<\;0$. In general, a negative differential resistance is a two-terminal component which can amplify,[3][12] converting DC power applied to its terminals to AC output power to amplify an AC signal applied to the same terminals.[9][13][14] They are used in electronic oscillators and amplifiers,[15] particularly at microwave frequencies.[6] Most microwave energy is produced with negative differential resistance devices.[16] They can also have hysteresis[17] and be bistable, and so are used in switching and memory circuits.[18] A device in which the "absolute resistance", the voltage divided by the current, is negative, is simply a power source,[19][20][21][22] converting power from some other source to electric power out of its terminals.

Because they are nonlinear, negative resistance devices have a more complicated behavior than the positive "ohmic" resistances usually encountered in electric circuits. Unlike most positive resistances, negative resistance varies depending on the voltage or current applied to the device, and a device can have negative resistance over only a limited portion of its voltage or current range.[6][11][23] Therefore there is no real "negative resistor" analogous to a positive resistor, which has a constant negative resistance over an arbitrarily wide range of current.

A Gunn diode, a semiconductor device with negative differential resistance used in electronic oscillators to generate microwaves

.

## Negative resistance devices

Electronic components with negative differential resistance include these devices:

Electric discharges through gases also exhibit negative differential resistance,[1][25] including these devices

In addition, active circuits with negative differential resistance can also be built with amplifying devices like transistors and op amps, using feedback.[6][25][35][36] A number of new experimental negative differential resistance materials and devices have been discovered in recent years.[37] The physical processes which cause negative resistance are diverse,[13][27][37] and each type of device has its own negative resistance characteristics, specified by its current–voltage curve.[11][25]

## Definitions

An I–V curve, showing the difference between static resistance (inverse slope of line B) and differential resistance (inverse slope of line C) at a point (A).

The resistance between two terminals of an electrical device or circuit is determined by its current–voltage (I–V) curve (characteristic curve), giving the current $\scriptstyle i\,$ through it for any given voltage $\scriptstyle v\,$ across it.[38] Most materials, including the ordinary (positive) resistances encountered in electrical circuits, obey Ohm's law; the current through them is proportional to the voltage over a wide range.[8][39][40] So the I–V curve of an ohmic resistance is a straight line through the origin with positive slope.[39] The resistance is the ratio of voltage to current, the inverse slope of the line (in I–V graphs where the voltage $\scriptstyle v\,$ is the independent variable) and is constant.[39]

Negative resistance occurs in a few nonlinear (nonohmic) devices.[41] In a nonlinear component the I–V curve is not a straight line,[8][42] so it does not obey Ohm's law.[41] Resistance can still be defined, but the resistance is not constant; it varies with the voltage or current through the device.[3][41][43] The resistance of such a nonlinear device can be defined in two ways,[40][42][43][44][45][46] which are equal for ohmic resistances:[20]

• Static resistance (also called chordal resistance,[39] absolute resistance or just resistance) – This is the common definition of resistance; the voltage divided by the current:[3][20][38][39][46]
$R_\mathrm{static} = {v \over i} \,$.
It is the inverse slope of the line (chord) from the origin through the point on the I–V curve.[8] In a power source, like a battery or electric generator, positive current flows out of the positive voltage terminal,[47] the opposite of a resistor, so from the passive sign convention $\scriptstyle i\,$ and $\scriptstyle v\,$ have opposite signs, representing points lying in the 2nd or 4th quadrant of the I–V plane (see diagram below). Thus power sources formally have negative static resistance ($\scriptstyle R_\text{static}\;<\;0$).[19][20][21][42][48][49][50][51] However this term is never used in practice, because the term "resistance" is only applied to passive components.[52][53][54] Static resistance determines the power dissipation in a component.[55][53] Passive devices, which consume electric power, have positive static resistance; while active devices, which produce electric power, do not.[19][20][21][42][48][56]
• Differential resistance (also called dynamic,[3][46] or incremental[8] resistance) – This is the derivative of the voltage with respect to the current; the ratio of a small change in voltage to the corresponding change in current,[10] the inverse slope of the I–V curve at a point:[39][43]
$r_\mathrm{diff} = \frac {dv}{di} \,$.
Differential resistance is only relevant to time-varying currents.[10] Points on the curve where the slope is negative (declining to the right), meaning an increase in voltage causes a decrease in current, have negative differential resistance ($\scriptstyle r_\text{diff}\;<\;0$).[3][10][20][42][57] Devices of this type can amplify signals,[3][12][15] and are what is usually meant by the term "negative resistance".[3][42]

Negative resistance, like positive resistance, is measured in ohms.

Fig. 1: I–V curve with negative differential resistance (red region).[20] The differential resistance $\scriptstyle r_\text{diff}\,$ at a point P is the inverse slope of the line tangent to the graph at that point

$r_\text{diff} = \frac {\Delta v}{\Delta i} = \frac {v_2 - v_1}{i_2 - i_1} \,$

Since $\scriptstyle \Delta v\;>\;0$ and $\scriptstyle \Delta i\;<\;0$, at point P $\scriptstyle r_\text{diff}\;<\;0$ .
Fig. 2: I–V curve of a power source.[20] In the 2nd quadrant (red region) current flows out of the positive terminal, so electric power flows out of the device into the circuit. For example at point P, $\scriptstyle v\;<\;0$ and $\scriptstyle i\;>\;0$, so
$R_\text{static} = {v \over i} < 0 \,$
Fig. 3: I–V curve of a negative linear or "active" resistance[6][22][58][59][60] (AR, red) contrasted with an ordinary ohmic resistance (OR, black). It has negative differential resistance and is an active device:
$R = {\Delta v \over \Delta i} = {v \over i} < 0 \,$
The quadrants of the I–V plane,[22][55] showing regions representing active devices (red).

## How it works

One way in which the different types of resistance can be distinguished is in the directions that current and electric power flow. The animations below summarize how the different types work:

 The voltage v and current i variables in an electrical component must be defined according to the passive sign convention; positive conventional current is defined to enter the positive voltage terminal; this means power P flowing from the circuit into the component is defined to be positive.[55][54] This applies to both DC and AC current. The diagram shows the directions for positive values of the variables. In a positive static resistance, $\scriptstyle R_\text{static}\;=\;v/i\;>\;0$, so v and i have the same sign.[22] Therefore conventional current (positive charge) flows through the device from the positive to the negative terminal, in the direction of the electric field E (decreasing potential).[55] $\scriptstyle P\;=\;vi\;>\;0$ so the charges lose potential energy doing work on the device, and electric power flows from the circuit into the device,[22][52] where it is converted to heat or some other form of energy (yellow). If AC voltage is applied, $\scriptstyle v$ and $\scriptstyle i$ periodically reverse direction, but the instantaneous $\scriptstyle i$ always flows from the higher potential to the lower potential. In a power source, $\scriptstyle v/i\;<\;0$.[20] so $\scriptstyle v$ and $\scriptstyle i$ have opposite signs.[22] This means current is forced to flow from the negative to the positive terminal.[20] The charges gain potential energy, so power flows out of the device into the circuit:[20][22] $\scriptstyle P\;=\;vi\;<\;0$. Work (yellow) must be done on the charges by some power source in the device to make them move in this direction against the force of the electric field. In a passive negative differential resistance, $\scriptstyle r_\text{diff}\;=\;\Delta v/\Delta i\;<\;0$, only the AC component of the current flows in the reverse direction. The static resistance is positive[8][10][44] so the current flows from positive to negative: $\scriptstyle P\;=\;vi\;>\;0$. But the current (rate of charge flow) decreases as the voltage increases. So when a time-varying (AC) voltage is applied in addition to a DC voltage (right), the time-varying current $\scriptstyle \Delta i\,$ and voltage $\scriptstyle \Delta v\,$ components have opposite signs, so $\scriptstyle P_\text{AC}\;=\;\Delta v\Delta i\;<\;0$.[35] This means the instantaneous $\scriptstyle \Delta i\,$ flows through the device in the direction of increasing $\scriptstyle \Delta v\,$, so AC power flows out of the device into the circuit. The device consumes DC power, some of which is converted to AC signal power which can be delivered to a load in the external circuit,[9][35] enabling the device to amplify the AC signal applied to it.[12]

## Types

rdiff > 0
Cannot amplify at port
rdiff < 0
Can amplify at port
Rstatic > 0
Passive:
Consumes
net power
Positive resistances:
• Resistors
• Ordinary diodes
• Most passive components
Passive negative differential resistances:
• Tunnel diodes
• Gunn diodes
• Gas-discharge tubes
Rstatic < 0
Active:
Produces
net power
Power sources:
• Batteries
• Generators
• Most active components
"Active resistors"
Positive feedback amplifiers used in:
• Feedback oscillators
• Negative impedance converters
• Active filters

In an electronic device, the differential resistance $\scriptstyle r_\text{diff}\,$, the static resistance $\scriptstyle R_\text{static}\,$, or both, can be nonpositive,[6][22] so there are three categories of devices (fig. 1–3 above, and table) which could be called "negative resistances".

The term "negative resistance" almost always means negative differential resistance $\scriptstyle r_\text{diff}\;<\;0$.[3][6][23][42] Negative differential resistance devices have unique capabilities: they can act as one-port amplifiers,[3][12][15][61] increasing the power of a time-varying signal applied to their port (terminals), or excite oscillations in a tuned circuit to make an oscillator.[35][61][62] They can also have hysteresis.[17][18] It is not possible for a device to have negative differential resistance without a power source,[49] and these devices can be divided into two categories depending on whether they get their power from an internal source or from their port:[6][18][35][62][63][64]

• Passive negative differential resistance devices (fig. 1 above): These are the most well-known type of "negative resistances"; passive two-terminal components whose intrinsic I–V curve has a downward "kink", causing the current to decrease with increasing voltage over a limited range.[63][64] The I–V curve, including the negative resistance region, lies in the 1st and 3rd quadrant of the plane[17] so the device has positive static resistance.[44] Examples are gas-discharge tubes, tunnel diodes, and Gunn diodes.[25] These devices have no power source and in general work by converting external DC power from their port to time varying (AC) power,[9] so they require a DC bias current applied to the port in addition to the signal.[35][62] To add to the confusion, some authors[23][25][62] call these "active" devices, since they can amplify. This category also includes a few three-terminal devices, such as the unijunction transistor.[25] They are covered in the Negative differential resistance section below.
• Active negative differential resistance devices (fig. 3): Circuits can be designed in which a positive voltage applied to the terminals will cause a proportional "negative" current; a current out of the positive terminal, the opposite of an ordinary resistor, over a limited range,[3][19][47][51][65] Unlike in the above devices, the downward-sloping region of the I–V curve passes through the origin, so it lies in the 2nd and 4th quadrants of the plane, meaning the device sources power.[6][22] Amplifying devices like transistors and op-amps with positive feedback can have this type of negative resistance,[6][35][36][47][64] and are used in feedback oscillators and active filters.[64][65] Since these circuits produce net power from their port, they must have an internal DC power source, or else a separate connection to an external power supply.[6][19][22][47] In circuit theory this is called an "active resistor".[22][50][56][66][67] It is often simply referred to as "negative resistance"[3][65] in electronics, although sometimes terms like "linear",[22][58] "absolute",[3] "ideal",[6] or "pure"[14] are added to distinguish this type from "passive" negative differential resistances. These are covered in the Active resistors section below.
A battery has negative static resistance[20][21] .(red) over its normal operating range, but positive differential resistance.

Occasionally ordinary power sources are referred to as "negative resistances"[21][42][48][68] (fig. 2). Although the "static" or "absolute" resistance $\scriptstyle R_\text{static}\,$ of active devices (power sources) can be considered negative (see Negative static resistance section below) most ordinary power sources (AC or DC), such as batteries, generators, and (non positive feedback) amplifiers, have positive differential resistance (their source resistance). Therefore these devices cannot function as one-port amplifiers or have the other capabilities of negative differential resistances.

Because of their ability to produce power and the air of mystery[65] surrounding them, much erroneous pseudoscientific information[69][70][71][72][73][74] has been written about negative resistance as a source of "free energy" in the "overunity" (perpetual motion) community.

## Negative static or "absolute" resistance

A positive static resistor (left) converts electric power to heat,[20] warming its surroundings. But a negative static resistance cannot function like this in reverse (right), converting ambient heat from the environment to electric power, because it would violate the second law of thermodynamics.[19][62][75][76][77][78] which requires a temperature difference to produce work. Therefore a negative static resistance must have some other source of power.

A point of some confusion is whether ordinary resistance ("static" or "absolute" resistance, $\scriptstyle R_\text{static}\;=\;v/i$) can be negative.[75][79] In electronics, the term "resistance" is customarily applied only to passive materials and components[53] – such as wires, resistors and diodes. These cannot have $\scriptstyle R_\text{static}\;<\;0$ as shown by Joule's law $\scriptstyle P\;=\;i^2 R_\text{static}$.[52] A passive device consumes electric power, so from the passive sign convention $\scriptstyle P\;\ge\;0$. Therefore from Joule's law $\scriptstyle R_\text{static}\;\ge\;0$.[20][48][52] In other words, no material can conduct electric current better than a "perfect" conductor with zero resistance.[8][80] For a passive device to have $\scriptstyle R_\text{static}\;=\;v/i\;<\;0$ would violate either conservation of energy[3] or the second law of thermodynamics,[19][62][75][78] (diagram). Therefore some authors[8][40][52][76] state that static resistance can never be negative.

From KVL, the static resistance of a power source (RS), such as a battery, is always equal to the negative of the static resistance of its load (RL).[48][64]

However it is easily shown that the ratio of voltage to current v/i at the terminals of any power source (AC or DC) is negative.[48] For electric power (potential energy) to flow out of a device into the circuit, charge must flow through the device in the direction of increasing potential energy, conventional current (positive charge) must move from the negative to the positive terminal.[19][20][60] So the direction of the instantaneous current is out of the positive terminal. This is opposite to the direction of current in a passive device defined by the passive sign convention so the current and voltage have opposite signs, and their ratio is negative

$R_\mathrm{static} = \frac {v}{i} < 0 \,$

This can also be proved from Joule's law[20][48][75]

$P = iv = i^2 R_{static} \,$

This shows that power can flow out of a device into the circuit ($\scriptstyle P\;<\;0$) if and only if $\scriptstyle R_\text{static}\;<\;0$.[6][20][21][22][49][56][75] Whether or not this quantity is referred to as "resistance" when negative is a matter of convention. Most authors[3][19][20][21][22][42][48][49][50][54][68][80][81] admit that the absolute resistance of power sources is negative, but most do not regard this as "resistance" in the same sense as positive resistances. The negative static resistance of a power source is a rather abstract and not very useful quantity, because it varies with the load. Due to conservation of energy it is always simply equal to the negative of the static resistance of the attached circuit (right).[48][64]

Work must be done on the charges by some source of energy in the device, to make them move toward the positive terminal against the electric field, so conservation of energy requires that negative static resistances have a source of power.[3][6][19][20][62] The power may come from an internal source which converts some other form of energy to electric power[56] as in a battery or generator, or from a separate connection to an external power supply circuit[19] as in an amplifying device like a transistor, vacuum tube, or op amp.

### Eventual passivity

A circuit cannot have negative static resistance (be active) over an infinite voltage or current range, because it would have to be able to produce infinite power.[6][11] Any active circuit or device with a finite power source is "eventually passive".[67][82][83] This property means if a large enough external voltage or current of either polarity is applied to it, its static resistance becomes positive[82]

$\exists V,I: |v| > V \text{ or } |i| > I \Rightarrow R_\mathrm{static} = v/i \ge 0 \,$
where $P_{max} = IV \,$ is the maximum power the device can produce.

Therefore the ends of the I–V curve will eventually turn and enter the 1st and 3rd quadrants.[6][83] Thus the range of the curve having negative static resistance is limited,[11] confined to a region around the origin. For example, applying a voltage to a generator or battery (graph, above) greater than its open-circuit voltage [6][84] will reverse the direction of current flow, making its static resistance positive so it consumes power. Similarly, applying a voltage to the negative impedance converter below greater than its power supply voltage Vs will cause the amplifier to saturate, also making its resistance positive.

## Negative differential resistance

In a device or circuit with negative differential resistance (NDR), in some part of the I–V curve the current decreases as the voltage increases:[6][39][44]

$r_\mathrm{diff} = \frac {dv}{di} < 0 \,$

The I–V curve is nonmonotonic (having peaks and troughs) with regions of negative slope representing negative differential resistance.[39]

Negative differential resistance
Voltage controlled (N type)
Current controlled (S type)

Passive negative differential resistances have positive static resistance;[3][8][39][44] they consume net power. Therefore the I–V curve is confined to the 1st and 3rd quadrants of the graph,[17] and passes through the origin. This requirement means (excluding some asymptotic cases) that the region(s) of negative resistance must be limited,[23][85] and surrounded by regions of positive resistance, and cannot include the origin.[3][11]

### Types

Negative differential resistances are commonly classified into two types:[6][18][25][64][85][86]

Most devices have a single negative resistance region. However devices with multiple separate negative resistance regions can also be fabricated.[37][90] These can have more than two stable states, and are of interest for use in digital circuits to implement multivalued logic.[37][90]

An intrinsic parameter used to compare different devices is the peak-to-valley current ratio (PVR),[37] the ratio of the current at the top of the negative resistance region to the current at the bottom (see graphs, above):

$\text{PVR} = i_1 / i_2 \,$

The larger this is, the larger the potential AC output for a given DC bias current, and therefore the greater the efficiency

### Amplification

Tunnel diode amplifier circuit. Since $\scriptstyle r\,>\,R$ the total resistance, the sum of the two resistances in series ($\scriptstyle R\;-\;r$) is negative, so an increase in input voltage will cause a decrease in current. The circuit operating point is the intersection between the diode curve (black) and the resistor load line $\scriptstyle R$ (blue).[91] A small increase in input voltage, $\scriptstyle v_i$ (green) moving the load line to the right, causes a large decrease in current through the diode and thus a large increase in the voltage across the diode $\scriptstyle v_o$.

A negative differential resistance device can amplify an AC signal applied to it[12][15] if the signal is biased with a DC voltage or current to lie within the negative resistance region of its I–V curve.[9][13][14]

The tunnel diode circuit is an example.[14][91] The tunnel diode TD has voltage controlled negative differential resistance.[24] The battery $\scriptstyle V_b$ adds a constant voltage (bias) across the diode so it operates in its negative resistance range, and provides power to amplify the signal.[14] Suppose the negative resistance at the bias point is $\scriptstyle \Delta v /\Delta i\,=\,-r$. For stability $\scriptstyle R\,$ must be less than $\scriptstyle r\,$.[60] Using the formula for a voltage divider, the AC output voltage is[14][91]

$v_o = \frac{-r}{R-r}v_i = \frac{r}{r-R}v_i \,$  so the voltage gain is  $G_v = \frac{r}{r-R} \,$

In a normal voltage divider, the resistance of each branch is less than the resistance of the whole, so the output voltage is less than the input. Here, due to the negative resistance, the total AC resistance $\scriptstyle r - R\,$ is less than the resistance of the diode alone $\scriptstyle r\,$ so the AC output voltage $\scriptstyle v_o$ is greater than the input $\scriptstyle v_i$.[14] The voltage gain $\scriptstyle G_v\,$ is greater than one, and increases without limit as $\scriptstyle R\,$ approaches $\scriptstyle r\,$.[14]

### Explanation of power gain

An AC voltage applied to a biased NDR. Since the change in current and voltage have opposite signs (shown by colors), the AC power dissipation ΔvΔi is negative, the device produces AC power rather than consuming it.
AC equivalent circuit of NDR attached to external circuit.[92] The NDR acts as a dependent AC current source of value Δi = Δv/r. Because the current and voltage are 180° out of phase, the instantaneous AC current Δi flows out of the terminal with positive AC voltage Δv. Therefore it adds to the AC source current ΔiS through the load R, increasing the output power.[92]

The diagrams illustrate how a biased negative differential resistance device can increase the power of a signal applied to it, amplifying it, although it only has two terminals. Due to the superposition principle the voltage and current at the device's terminals can be divided into a DC bias component ($\scriptstyle V_{bias},\;I_{bias}$) and an AC component ($\scriptstyle \Delta v,\;\Delta i$).

$v(t) = V_\text{bias} + \Delta v(t)\,$
$i(t) = I_\text{bias} + \Delta i(t)\,$

Since a positive change in voltage $\scriptstyle \Delta v\,$ causes a negative change in current $\scriptstyle \Delta i\,$, the AC current and voltage in the device are 180° out of phase.[9][28][60][93] This means in the AC equivalent circuit (right), the instantaneous AC current Δi flows through the device in the direction of increasing AC potential Δv, as it would in a generator.[60] Therefore the AC power dissipation is negative; AC power is produced by the device and flows into the external circuit.[94]

$P_\text{AC} = \Delta v \Delta i = r_\text{diff}|\Delta i|^2 < 0 \,$

With the proper external circuit, the device can increase the AC signal power delivered to a load, serving as an amplifier,[14][60] or excite oscillations in a resonant circuit to make an oscillator. Unlike in a two port amplifying device such as a transistor or op amp, the amplified signal leaves the device through the same two terminals (port) as the input signal enters.[95]

In a passive device, the AC power produced comes from the input DC bias current,[44] the device absorbs DC power, some of which is converted to AC power by the nonlinearity of the device, amplifying the applied signal. Therefore the output power is limited by the bias power[44]

$|P_\text{AC}| \le I_\text{bias} V_\text{bias} \,$

The negative differential resistance region cannot include the origin, because it would then be able to amplify a signal with no applied DC bias current, producing AC power with no power input.[3][11][44] The device also dissipates some power as heat, equal to the difference between the DC power in and the AC power out.

The device may also have reactance and therefore the phase difference between current and voltage may differ from 180° and may vary with frequency.[64][96] As long as the real component of the impedance is negative (phase angle between 90° and 270°),[93] the device will have negative resistance and can amplify.[96][97]

The maximum AC output power is limited by size of the negative resistance region ($\scriptstyle v_1,\; v_2,\; i_1,\; and\; i_2$ in graphs above)[44][98]

$P_{AC(rms)} \le \frac{1}{8}(v_2 - v_1)(i_1 - i_2) \,$

### Reflection coefficient

General (AC) model of a negative resistance circuit: a negative differential resistance device $\scriptstyle Z_\text{N}(j\omega)\;$, connected to an external circuit represented by $\scriptstyle Z_\text{L}(j\omega)\,$

The reason that the output signal can leave a negative resistance through the same port that the input signal enters is that from transmission line theory, the AC voltage or current at the terminals of a component can be divided into two oppositely moving waves, the incident wave $\scriptstyle V_I\,$, which travels toward the device, and the reflected wave $\scriptstyle V_R\,$, which travels away from the device.[99] A negative differential resistance in a circuit can amplify if the magnitude of its reflection coefficient $\scriptstyle \Gamma \,$, the ratio of the reflected wave to the incident wave, is greater than one.[23][94]

$|\Gamma| \equiv \bigg|\frac{V_R}{V_I}\bigg| > 1 \,$   where   $\Gamma \equiv \frac {Z_N - Z_L}{Z_N + Z_L} \,$

The "reflected" (output) signal has larger amplitude than the incident; the device has "reflection gain".[23] The reflection coefficient is determined by the AC impedance of the negative resistance device, $\scriptstyle Z_N(j\omega)\,=\,R_N\,+\,jX_N$, and the impedance of the circuit attached to it, $\scriptstyle Z_L(j\omega)\,=\,R_L\,+\,jX_L$.[94] If $\scriptstyle R_N\,<\,0$ and $\scriptstyle R_L\,>\,0\,$ then $\scriptstyle |\Gamma|\,>\,0\,$ and the device will amplify. On the Smith chart, a graphical aide widely used in the design of high frequency circuits, negative differential resistance corresponds to points outside the unit circle $\scriptstyle |\Gamma|\,=\,1\,$, the boundary of the conventional chart, so special "expanded" charts must be used.[23][100]

### Stability conditions

Because it is nonlinear, a circuit with negative differential resistance can have multiple equilibrium points (possible DC operating points), which lie on the I–V curve.[101] An equilibrium point will be stable, so the circuit converges to it within some neighborhood of the point, if its poles are in the left half of the s plane (LHP), while a point is unstable, causing the circuit to oscillate or "latch up" (converge to another point), if its poles are on the axis or right half plane (RHP), respectively.[102][103] The equilibrium points are determined by the DC bias circuit, and their stability is determined by the AC impedance $\scriptstyle Z_L(j\omega)\,$ of the external circuit. However, because of the different shapes of the curves, the condition for stability is different for VCNR and CCNR types of negative resistance:[95][104]

• In a CCNR (S-type) negative resistance, the resistance function $\scriptstyle R_N\,$ is single-valued. Therefore stability is determined by the poles of the circuit's impedance equation:$\scriptstyle Z_L(j\omega)\;+\;Z_N(j\omega)\;=\;0\,$.[105][106]
For nonreactive circuits ($\scriptstyle X_L\;=\;X_N\;=\;0\,$) a sufficient condition for stability is that the total resistance is positive[107]
$Z_L + Z_N = R_L + R_N = R_L - r > 0 \,$
so the CCNR is stable for[18][85][104]
 $R_L\;>\;r$.
Since CCNRs are stable with no load at all, they are called "open circuit stable".[85][87][95][108][note 1]
• In a VCNR (N-type) negative resistance, the conductance function $\scriptstyle G_N\;=\;1/R_N$ is single-valued. Therefore stability is determined by the poles of the admittance equation $\scriptstyle Y_L(j\omega)\;+\;Y_N(j\omega)\;=\;0$.[105][106] For this reason the VCNR is sometimes referred to as a negative conductance.
As above, for nonreactive circuits a sufficient condition for stability is that the total conductance in the circuit is positive[107]
$Y_L + Y_N = G_L + G_N = {1 \over R_L} + {1 \over R_N} = {1 \over R_L} + {1 \over -r} > 0 \,$
${1 \over R_L} > {1 \over r}\,$
so the VCNR is stable for[18][104]
 $R_L\;<\;r$.
Since VCNRs are even stable with a short-circuited output, they are called "short circuit stable".[85][87][108][note 1]

For general negative resistance circuits with reactance, the stability must be determined by standard tests like the Nyquist stability criterion.[109] Alternatively, in high frequency circuit design, the values of $\scriptstyle Z_L(j\omega)$ for which the circuit is stable are determined by a graphical technique using "stability circles" on a Smith chart.[23]

### Operating regions and applications

For simple nonreactive negative resistance devices with $\scriptstyle R_N\;=\;-r$ and $\scriptstyle X_N\;=\;0$ the different operating regions of the device can be illustrated by load lines on the I–V curve[85] (see graphs).

VCNR (N type) load lines and stability regions
CCNR (S type) load lines and stability regions

The DC load line (DCL) is a straight line determined by the DC bias circuit, with equation

$V = V_S - IR\,$

where $\scriptstyle V_S$ is the DC bias supply voltage and R is the resistance of the supply. The possible DC operating point(s) (Q points) occur where the DC load line intersects the I–V curve. For stability[110]

• VCNRs require a low impedance bias ($\scriptstyle R\;<\;r$), such as a voltage source.
• CCNRs require a high impedance bias ($\scriptstyle R\;>\;r$) such as a current source, or voltage source in series with a high resistance.

The AC load line (L1L3) is a straight line through the Q point whose slope is the differential (AC) resistance $\scriptstyle R_L\,$ facing the device. Increasing $\scriptstyle R_L\,$ rotates the load line counterclockwise. The circuit operates in one of three possible regions, depending on $\scriptstyle R_L\,$.[85]

• Stable region (green) (illustrated by line L1): When the load line lies in this region, it intersects the I–V curve at one point Q1.[85] For nonreactive circuits it is a stable equilibrium (poles in the LHP) so the circuit is stable. Negative resistance amplifiers operate in this region. However, due to hysteresis, with an energy storage device like a capacitor or inductor the circuit can become unstable to make a nonlinear relaxation oscillator (astable multivibrator) or a monostable multivibrator.[111]
• VCNRs are stable when $\scriptstyle R_L\;<\;r$.
• CCNRs are stable when $\scriptstyle R_L\;>\;r$.
• Unstable point (Line L2): When $\scriptstyle R_L\;=\;r$ the load line is tangent to the I–V curve. The total differential (AC) resistance of the circuit is zero (poles on the axis), so it is unstable and with a tuned circuit can oscillate. Linear oscillators operate at this point. Practical oscillators actually start in the unstable region below, with poles in the RHP. But as the amplitude increases the oscillations become nonlinear, and due to eventual passivity the negative resistance r decreases with increasing amplitude, so the oscillations stabilize at an amplitude where[112] $\scriptstyle r\;=\;R_L$.
• Bistable region (red) (illustrated by line L3): In this region the load line can intersect the I–V curve at three points.[6][85] The center point (Q1) is a point of unstable equilibrium (poles in the RHP), while the two outer points, Q2 and Q3 are stable equilibria. So with correct biasing the circuit can be bistable, it will converge to one of the two points Q2 or Q3 and can be switched between them with an input pulse. Switching circuits like flip-flops (bistable multivibrators) and Schmidt triggers operate in this region.
• VCNRs can be bistable when $\scriptstyle R_L\;>\;r$
• CCNRs can be bistable when $\scriptstyle R_L\;<\;r$

## Active resistors – negative resistance from feedback

Typical I–V curves of "active" negative resistances:[6][59][113] N-type (left), and S-type (center), generated by feedback amplifiers. These have negative differential resistance (red region) and produce power (grey region). Applying a large enough voltage or current of either polarity to the port moves the device into its nonlinear region where saturation of the amplifier causes the differential resistance to become positive (black portion of curve), and above the supply voltage rails $\scriptstyle \pm V_S\,$ the static resistance becomes positive and the device consumes power. The negative resistance depends on the loop gain $\scriptstyle A\beta \,$ (right).
An example of an amplifier with positive feedback that has negative resistance at its input. The input current i is
$i = {{v - Av} \over R_1} + {v \over R_\text{in}}\,$
so the input resistance is
$R = {v \over i} = {R_1 \over {1 + R_1/R_\text{in} - A}}\,$ If $A > 1 + R_1/R_\text{in} \,$ it will have negative input resistance.

In addition to the passive devices with intrinsic negative differential resistance above, circuits with amplifying devices like transistors or op amps can have negative resistance at their ports.[3][35] The input or output impedance of an amplifier with enough positive feedback applied to it can be negative.[36][61][114][115] If $\scriptstyle R_i\,$ is the input resistance of the amplifier without feedback, $\scriptstyle A\,$ is the amplifier gain, and $\scriptstyle \beta(j\omega)\,$ is the transfer function of the feedback path, the input resistance with positive shunt feedback is[3][116]

$R_\text{if} = \frac {R_\text{i} }{1 - A\beta} \,$

So if the loop gain $\scriptstyle A\beta \,$ is greater than one, $\scriptstyle R_{if}\,$ will be negative. The circuit acts like a "negative linear resistor"[3][51][58][117] over a limited range,[64] with I–V curve having a straight line segment through the origin with negative slope (see graphs).[6][22][37][47][59][113] It has both negative differential resistance and is active

${\Delta v \over \Delta i} = {v \over i} = R_\text{if} < 0 \,$

and thus obeys Ohm's law with a negative proportionality,[6][37][65] over its linear range (such amplifiers can also have more complicated negative resistance I–V curves that don't pass through the origin).

These are often called "active resistors".[22][50][56][66][67] Applying a voltage across the terminals causes a proportional current out of the positive terminal, the opposite of an ordinary resistor.[47][51][65] For example, connecting a battery to the terminals would cause the battery to charge rather than discharge.[19]

Considered as one-port devices, these circuits function similarly to the passive negative differential resistance components above,[6] and like them can be used to make one-port amplifiers and oscillators[3][12] with the advantages that (1) because they are active devices they do not require an external DC bias to provide power, and can be DC coupled; (2) the amount of negative resistance can be varied by adjusting the loop gain; and (3) they can be linear circuit elements;[58][64] the voltage is proportional to the current, so they don't cause harmonic distortion. The I–V curve can have voltage-controlled ("N" type) or current-controlled ("S" type) negative resistance, depending on whether the feedback loop is connected in "shunt" or "series".[47]

Negative reactances (below) can also be created, so feedback circuits can be used to create "active" linear circuit elements, resistors, capacitors, and inductors, with negative values.[6][35][65] They are widely used in active filters[58][64] because they can create transfer functions that cannot be realized with positive circuit elements.[118] Examples of circuits with this type of negative resistance are the negative impedance converter (NIC), gyrator, Deboo integrator,[58][119] frequency dependent negative resistance (FDNR),[65] and generalized immittance converter (GIC).[6][64][105][120]

### Feedback oscillators

If an LC circuit is connected across the input of a positive feedback amplifier like that above, the negative differential input resistance $\scriptstyle R_\text{if}$ can cancel the positive loss resistance $\scriptstyle r_\text{loss}$ inherent in the tuned circuit.[121] If $\scriptstyle R_\text{if}\;=\;-r_\text{loss}$ this will create in effect a tuned circuit with zero AC resistance (poles on the axis).[62][114] Spontaneous oscillation will be excited in the tuned circuit at its resonant frequency, sustained by the power from the amplifier. This is how feedback oscillators such as Hartley or Colpitts oscillators work.[63][122] This negative resistance model is an alternate way of analyzing feedback oscillator operation.[16][111][115][123][124][125] All linear oscillator circuits have negative resistance[93][111][124] although in most feedback oscillators the tuned circuit is an integral part of the feedback network, so the circuit does not have negative resistance at all frequencies but only near the oscillation frequency.

### Q enhancement

A tuned circuit connected to a negative resistance which cancels some but not all of its parasitic loss resistance, so $\scriptstyle |R_\text{if}|\;<\;r_\text{loss}$ will not oscillate, but the negative resistance will decrease the damping in the circuit (moving its poles toward the axis), increasing its Q factor so it has a narrower bandwidth and more selectivity.[121][126][127][128] Q enhancement, also called regeneration, was first used in the regenerative radio receiver invented by Edwin Armstrong in 1912[114][127] and later in "Q multipliers".[129] Today it is widely used in active filters.[128] For example, RF integrated circuits use integrated inductors to save space, consisting of a spiral conductor fabricated on chip. These have high losses and low Q, so to create high Q tuned circuits their Q is increased by applying negative resistance.[126][128]

### Chaotic circuits

Circuits which exhibit chaotic behavior can be considered quasi-periodic or nonperiodic oscillators, and like all oscillators require a negative resistance in the circuit to provide power.[130] Chua's circuit, a simple nonlinear circuit widely used as the standard example of a chaotic system, requires a nonlinear active resistor component, sometimes called Chua's diode.[130] This is usually synthesized using a negative impedance converter circuit.[130]

### Negative impedance converter

Negative impedance converter (left) and I–V curve (right). It has negative differential resistance in red region and sources power in grey region.

A common example of an "active resistance" circuit is the negative impedance converter (NIC)[51][65][122][131][132] shown in the diagram. The two resistors $\scriptstyle R_\text{1}$ and the op amp constitute a negative feedback non-inverting amplifier with gain of 2.[6][122] The output voltage of the op-amp is

$v_o = v(R_1 + R_1)/R_1 = 2v \,$

So if a voltage $\scriptstyle v\,$ is applied to the input, the same voltage is applied "backwards" across $\scriptstyle Z$, causing current to flow through it out of the input.[65] The current is

$i = \frac {v - v_o}{Z} = \frac {v - 2v}{Z} = - \frac {v}{Z} \,$

So the input impedance to the circuit is[84][132]

$z_\text{in} = \frac {v}{i} = -Z \,\!$

The circuit converts the impedance $\scriptstyle Z$ to its negative. If $\scriptstyle Z$ is a resistor of value $\scriptstyle R$, within the linear range of the op amp $\scriptstyle V_\text{S}/2\;<\;v\;<\;-V_\text{S}/2$ the input impedance acts like a linear "negative resistor"[6] of value $\scriptstyle -R$.[65] The input port of the circuit is connected into another circuit as if it was a component. An NIC can cancel undesired positive resistance in another circuit,[133] for example they were originally developed to cancel resistance in telephone cables, serving as repeaters.[122]

### Negative capacitance and inductance

By replacing $\scriptstyle Z$ in the above circuit with a capacitor ($\scriptstyle C$) or inductor ($\scriptstyle L$), negative capacitances and inductances can also be synthesized.[35][65][132] A negative capacitance will have an I–V relation and an impedance $\scriptstyle Z_\text{C}(j\omega)$ of[132]

$i = -C {dv \over dt} \qquad\qquad Z_C = -1/j\omega C \,$

where $\scriptstyle C\;>\;0$. Applying a positive current to a negative capacitance will cause it to discharge; its voltage will decrease. Similarly, a negative inductance will have an I–V characteristic and impedance $\scriptstyle Z_\text{L}(j\omega)$ of

$v = -L {di \over dt} \qquad\qquad Z_L = -j\omega L \,$

A circuit having negative capacitance or inductance can be used to cancel unwanted positive capacitance or inductance in another circuit.[65] NIC circuits were used to cancel reactance on telephone cables.

There is also another way of looking at them. In a negative capacitance the current will be 180° opposite in phase to the current in a positive capacitance. Instead of leading the voltage by 90° it will lag the voltage by 90°, as in an inductor.[65][132] Therefore a negative capacitance acts like an inductance in which the impedance has a reverse dependence on frequency ω; decreasing instead of increasing like a real inductance[65][132] Similarly a negative inductance acts like a capacitance that has an impedance which increases with frequency. Negative capacitances and inductances are "non-Foster" circuits which violate Foster's reactance theorem.[134] One application being researched is to create an active matching network which could match an antenna to a transmission line over a broad range of frequencies, rather than just a single frequency as with current networks.[135] This would allow the creation of small compact antennas that would have broad bandwidth,[135] exceeding the Chu–Harrington limit.

## Negative resistance oscillators

An oscillator consisting of a Gunn diode inside a cavity resonator. The negative resistance of the diode excites microwave oscillations in the cavity, which radiate through the aperture into a waveguide (not shown).

Negative differential resistance devices are widely used to make electronic oscillators.[9][25][136] In a negative resistance oscillator, a negative differential resistance device such as an IMPATT diode, Gunn diode, or microwave vacuum tube is connected across an electrical resonator such as an LC circuit, a quartz crystal, dielectric resonator or cavity resonator[124] with a DC source to bias the device into its negative resistance region and provide power.[57][82] A resonator such as an LC circuit is "almost" an oscillator; it can store oscillating electrical energy, but because all resonators have internal resistance or other losses the oscillations are damped and decay to zero.[44][62][122] The negative resistance cancels the positive resistance of the resonator, creating in effect a lossless resonator, in which spontaneous continuous oscillations occur at the resonator's resonant frequency.[44][62]

### Uses

Negative resistance oscillators are mainly used at high frequencies in the microwave range or above, since feedback oscillators function poorly at these frequencies.[16][123] Microwave diodes are used in low- to medium-power oscillators for applications such as radar speed guns, and local oscillators for satellite receivers. They are a widely used source of microwave energy, and virtually the only solid-state source of millimeter wave[89] and terahertz energy[136] Negative resistance microwave vacuum tubes such as magnetrons produce higher power outputs,[124] in such applications as radar transmitters and microwave ovens. Lower frequency relaxation oscillators can be made with unijunction transistors and gas-discharge lamps such as neon lamps.[137]

The negative resistance oscillator model is not limited to one-port devices like diodes but can also be applied to feedback oscillator circuits with two port devices such as transistors and tubes.[111][123][124][125] In addition, in modern high frequency oscillators, transistors are increasingly used as one-port negative resistance devices like diodes. At microwave frequencies, transistors with certain loads applied to one port can become unstable due to internal feedback and show negative resistance at the other port.[35][97][123] So high frequency transistor oscillators are designed by applying a reactive load to one port to give the transistor negative resistance, and connecting the other port across a resonator to make a negative resistance oscillator as described below.[123][125]

### Gunn diode oscillator

Gunn diode oscillator circuit
AC equivalent circuit
DCL: DC load line, which sets the Q point.
SSL: negative resistance during startup while amplitude is small. Since $\scriptstyle r\;<\;R$ poles are in RHP and amplitude of oscillations increases.
LSL: large-signal load line. When the current swing approaches the edges of the negative resistance region (green), the sine wave peaks are distorted ("clipped") and $\scriptstyle r$ decreases until it equals $\scriptstyle R$.

The common Gunn diode oscillator (circuit diagrams)[44] illustrates how negative resistance oscillators work. The diode D has voltage controlled ("N" type) negative resistance and the voltage source $\scriptstyle V_\text{b}$ biases it into its negative resistance region where its differential resistance is $\scriptstyle dv/di\;=\;-r$. The choke RFC prevents AC current from flowing through the bias source.[44] $\scriptstyle R$ is the equivalent resistance due to damping and losses in the series tuned circuit $\scriptstyle LC$, plus any load resistance. Analyzing the AC circuit with Kirchhoff's Voltage Law gives a differential equation for $\scriptstyle i(t)$, the AC current[44]

$\frac {d^2 i}{dt^2} + \frac {R - r}{L}\frac {di}{dt} + \frac {1}{LC}i = 0 \,$

Solving this equation gives a solution of the form[44]

$i(t) = i_0 e^{\alpha t} \cos(\omega t + \phi) \,$     where    $\alpha = \frac{r - R}{2L} \quad \omega = \sqrt{\frac {1}{LC} - \Big(\frac {r - R}{2L}\Big)^2} \,$

This shows that the current through the circuit, $\scriptstyle i(t)$, varies with time about the DC Q point, $\scriptstyle I_\text{bias}$. When started from a nonzero initial current $\scriptstyle i(t)\;=\;i_0$ the current oscillates sinusoidally at the resonant frequency ω of the tuned circuit, with amplitude either constant, increasing, or decreasing exponentially, depending on the value of α. Whether the circuit can sustain steady oscillations depends on the balance between $\scriptstyle R$ and $\scriptstyle r$, the positive and negative resistance in the circuit:[44]

1. $r < R \Rightarrow \alpha < 0\,$: (poles in left half plane) If the diode's negative resistance is less than the positive resistance of the tuned circuit, the damping is positive. Any oscillations in the circuit will lose energy as heat in the resistance $\scriptstyle R$ and die away exponentially to zero, as in an ordinary tuned circuit.[62] So the circuit does not oscillate.
2. $r = R \Rightarrow \alpha = 0\,$: (poles on axis) If the positive and negative resistances are equal, the net resistance is zero, so the damping is zero. The diode adds just enough energy to compensate for energy lost in the tuned circuit and load, so oscillations in the circuit, once started, will continue at a constant amplitude.[62] This is the condition during steady-state operation of the oscillator.
3. $r > R \Rightarrow \alpha > 0\,$: (poles in right half plane) If the negative resistance is greater than the positive resistance, damping is negative, so oscillations will grow exponentially in energy and amplitude.[62] This is the condition during startup.

Practical oscillators are designed in region (3) above, with net negative resistance, to get oscillations started.[125] A widely used rule of thumb is to make $\scriptstyle R\;=\;r/3$.[23][138] When the power is turned on, electrical noise in the circuit provides a signal $\scriptstyle i_0$ to start spontaneous oscillations, which grow exponentially. However, the oscillations cannot grow forever; the nonlinearity of the diode eventually limits the amplitude.

At large amplitudes the circuit is nonlinear, so the linear analysis above does not strictly apply and differential resistance is undefined; but the circuit can be understood by considering $\scriptstyle r$ to be the "average" resistance over the cycle. As the amplitude of the sine wave exceeds the width of the negative resistance region and the voltage swing extends into regions of the curve with positive differential resistance, the average negative differential resistance $\scriptstyle r$ becomes smaller, and thus the total resistance $\scriptstyle R\;-\;r$ and the damping $\scriptstyle \alpha$ becomes less negative and eventually turns positive. Therefore the oscillations will stabilize at the amplitude at which the damping becomes zero, which is when $\scriptstyle r\;=\;R$.[44]

Gunn diodes have negative resistance in the range −5 to −25 ohms.[139] In oscillators where $\scriptstyle R$ is close to $\scriptstyle r$; just small enough to allow the oscillator to start, the voltage swing will be mostly limited to the linear portion of the I–V curve, the output waveform will be nearly sinusoidal and the frequency will be most stable. In circuits in which $\scriptstyle R$ is far below $\scriptstyle r$, the swing extends further into the nonlinear part of the curve, the clipping distortion of the output sine wave is more severe,[138] and the frequency will be increasingly dependent on the supply voltage.

### Types of circuit

Negative resistance oscillator circuits can be divided into two types, which are used with the two types of negative differential resistance – voltage controlled (VCNR), and current controlled (CCNR)[100][110]

• Negative resistance (voltage controlled) oscillator: Since VCNR ("N" type) devices require a low impedance bias and are stable for load impedances less than r,[110] the ideal oscillator circuit for this device has the form shown at top right, with a voltage source Vbias to bias the device into its negative resistance region, and parallel resonant circuit load LC. The resonant circuit has high impedance only at its resonant frequency, so the circuit will be unstable and oscillate only at that frequency.
• Negative conductance (current controlled) oscillator: CCNR ("S" type) devices, in contrast, require a high impedance bias and are stable for load impedances greater than r.[110] The ideal oscillator circuit is like that at bottom right, with a current source bias Ibias (which may consist of a voltage source in series with a large resistor) and series resonant circuit LC. The series LC circuit has low impedance only at its resonant frequency and so will only oscillate there.

### Conditions for oscillation

Most oscillators are more complicated than the Gunn diode example, since both the active device and the load may have reactance (X) as well as resistance (R). Modern negative resistance oscillators are designed by a frequency domain technique due to K. Kurokawa.[97][125][140] The circuit diagram is imagined to be divided by a "reference plane" (red) which separates the negative resistance part, the active device, from the positive resistance part, the resonant circuit and output load (right).[141] The complex impedance of the negative resistance part $\scriptstyle Z_N = R_N(I, \omega) + jX_N(I, \omega) \,$ depends on frequency ω but is also nonlinear, in general declining with the amplitude of the AC oscillation current I; while the resonator part $\scriptstyle Z_L = R_L(\omega) + jX_L(\omega) \,$ is linear, depending only on frequency.[97][124][141] The circuit equation is $\scriptstyle (Z_N + Z_L)I = 0\,$ so it will only oscillate (have nonzero I) at the frequency ω and amplitude I for which the total impedance $\scriptstyle Z_N + Z_L \,$ is zero.[97] This means the magnitude of the negative and positive resistances must be equal, and the reactances must be conjugate[94][124][125][141]

$R_N \le -R_L\,$    and    $X_N = -X_L \,$

For steady-state oscillation the equal sign applies. During startup the inequality applies, because the circuit must have excess negative resistance for oscillations to start.[94][97][125]

Alternately, the condition for oscillation can be expressed using the reflection coefficient.[94] The voltage waveform at the reference plane can be divided into a component V1 travelling toward the negative resistance device and a component V2 travelling in the opposite direction, toward the resonator part. The reflection coefficient of the active device $\scriptstyle \Gamma_N = V_2/V_1 \,$ is greater than one, while that of the resonator part $\scriptstyle \Gamma_L = V_1/V_2 \,$ is less than one. During operation the waves are reflected back and forth in a round trip so the circuit will oscillate only if[94][124][141]

$|\Gamma_N \Gamma_L| \ge 1 \,$

As above, the equality gives the condition for steady oscillation, while the inequality is required during startup to provide excess negative resistance. The above conditions are analogous to the Barkhausen criterion for feedback oscillators; they are necessary but not sufficient,[125] so there are some circuits that satisfy the equations but do not oscillate. Kurokawa also derived more complicated sufficient conditions,[140] which are often used instead.[97][125]

## Negative resistance amplifiers

Negative differential resistance devices such as Gunn and IMPATT diodes are also used to make amplifiers, particularly at microwave frequencies, but not as commonly as oscillators.[95] Because negative resistance devices have only one port (two terminals), unlike two-port devices such as transistors, the outgoing amplified signal has to leave the device by the same terminals as the incoming signal enters it.[13][95] Without some way of separating the two signals, a negative resistance amplifier is bilateral; it amplifies in both directions, so it suffers from sensitivity to load impedance and feedback problems.[95] To separate the input and output signals, many negative resistance amplifiers use nonreciprocal devices such as isolators and directional couplers.[95]

### Reflection amplifier

AC equivalent circuit of reflection amplifier
8–12 GHz microwave amplifier consisting of two cascaded tunnel diode reflection amplifiers

One widely used circuit is the reflection amplifier in which the separation is accomplished by a circulator.[95][142][143][144] A circulator is a nonreciprocal solid-state component with three ports (connectors) which transfers a signal applied to one port to the next in only one direction, port 1 to port 2, 2 to 3, and 3 to 1. In the reflection amplifier diagram the input signal is applied to port 1, a biased VCNR negative resistance diode N is attached through a filter F to port 2, and the output circuit is attached to port 3. The input signal is passed from port 1 to the diode at port 2, but the outgoing "reflected" amplified signal from the diode is routed to port 3, so there is little coupling from output to input. The characteristic impedance $\scriptstyle Z_0$ of the input and output transmission lines, usually 50Ω, is matched to the port impedance of the circulator. The purpose of the filter F is to present the correct impedance to the diode to set the gain. At radio frequencies NR diodes are not pure resistive loads and have reactance, so a second purpose of the filter is to cancel the diode reactance with a conjugate reactance to prevent standing waves.[144][145]

The filter has only reactive components and so does not absorb any power itself, so power is passed between the diode and the ports without loss. The input signal power to the diode is

$P_\text{in} = V_I^2 / R_1\,$

The output power from the diode is

$P_\text{out} = V_R^2 / R_1\,$

So the power gain $\scriptstyle G_P$ of the amplifier is the square of the reflection coefficient[142][144][145]

$G_\text{P} = {P_\text{out} \over P_\text{in}} = {V_R^2 \over V_I^2} = |\Gamma|^2\,$
$|\Gamma|^2 = \Bigg|{Z_N - Z_1 \over Z_N + Z_1}\Bigg|^2\,$
$|\Gamma|^2 = \Bigg|{R_N + jX_N - (R_1 + jX_1)\over R_N + jX_N + R_1 + jX_1}\Bigg|^2\,$

$\scriptstyle R_\text{N}$ is the negative resistance of the diode −r. Assuming the filter is matched to the diode so $\scriptstyle X_1\;=\;-X_N$[144] then the gain is

$G_\text{P} = |\Gamma|^2 = \Big|{r + R_1 \over r - R_1}\Big|^2\,$

The VCNR reflection amplifier above is stable for $\scriptstyle R_1\;<\;r$.[144] while a CCNR amplifier is stable for $\scriptstyle R_1\;>\;r$. It can be seen that the reflection amplifier can have unlimited gain, approaching infinity as $\scriptstyle R_\text{1}$ approaches the point of oscillation at $\scriptstyle r$.[144] This is a characteristic of all NR amplifiers,[143] contrasting with the behavior of two-port amplifiers, which generally have limited gain but are often unconditionally stable. In practice the gain is limited by the backward "leakage" coupling between circulator ports.

Masers and parametric amplifiers are extremely low noise NR amplifiers that are also implemented as reflection amplifiers; they are used in applications like radio telescopes.[145]

## Switching circuits

Negative differential resistance devices are also used in switching circuits in which the device operates nonlinearly, changing abruptly from one state to another, with hysteresis.[17] The advantage of using a negative resistance device is that a relaxation oscillator, flip-flop or memory cell can be built with a single active device,[90] whereas the standard logic circuit for these functions, the Eccles-Jordan multivibrator, requires two active devices (transistors). Three switching circuits built with negative resistances are

• Astable multivibrator – a circuit with two unstable states, in which the output periodically switches back and forth between the states. The time it remains in each state is determined by the time constant of an RC circuit. Therefore it is a relaxation oscillator, and can produce square waves or triangle waves.
• Monostable multivibrator – is a circuit with one unstable state and one stable state. When in its stable state a pulse is applied to the input, the output switches to its other state and remains in it for a period of time dependent on the time constant of the RC circuit, then switches back to the stable state. Thus the monostable can be used as a timer or delay element.
• Bistable multivibrator or flip flop – is a circuit with two stable states. A pulse at the input switches the circuit to its other state. Therefore bistables can be used as memory circuits, and digital counters.

## Other applications

### Neuronal models

Some instances of neurons display regions of negative slope conductances (RNSC) in voltage-clamp experiments.[146] The negative resistance here is implied were one to consider the neuron a typical Hodgkin–Huxley style circuit model.

## History

Negative resistance was first recognized during investigations of electric arcs, which were used for lighting during the 19th century.[147] In 1881 Alfred Niaudet[148] had observed that the voltage across arc electrodes decreased temporarily as the arc current increased, but many researchers thought this was a secondary effect due to temperature.[149] The term "negative resistance" was applied by some to this effect, but the term was controversial because it was known that the resistance of a passive device could not be negative.[75][149][150] Beginning in 1895 Hertha Ayrton, extending her husband William's research with a series of meticulous experiments measuring the I–V curve of arcs, established that arcs had negative resistance, igniting controversy.[33][149][151] Frith and Rodgers in 1896[149][152] with the support of the Ayrtons[33] introduced the concept of differential resistance, dv/di, and it was slowly accepted that arcs had negative differential resistance. In recognition of her research, Hertha Ayrton became the first woman voted for induction into the Institute of Electrical Engineers.[151]

### Arc transmitters

George Francis Fitzgerald first realized in 1892 that if the damping resistance in a resonant circuit could be made zero or negative, it would produce continuous oscillations.[147][153] In the same year Elihu Thomson built a negative resistance oscillator by connecting an LC circuit to the electrodes of an arc,[112][154] perhaps the first example of an electronic oscillator. William Duddell, a student of Ayrton at London Central Technical College, brought Thomson's arc oscillator to public attention.[112][147][151] Due to its negative resistance, the current through an arc was unstable, and arc lights would often produce hissing, humming, or even howling noises. In 1899, investigating this effect, Duddell connected an LC circuit across an arc and the negative resistance excited oscillations in the tuned circuit, producing a musical tone from the arc.[112][147][151] To demonstrate his invention Duddell wired several tuned circuits to an arc and played a tune on it.[147][151] Duddell's "singing arc" oscillator was limited to audio frequencies.[112] However in 1903 Danish engineers Valdemar Poulsen and P. O. Pederson increased the frequency into the radio range by operating the arc in a hydrogen atmosphere in a magnetic field, inventing the Poulsen arc radio transmitter, which was widely used until the 1920s.[112][147]

### Vacuum tubes

By the early 20th century, although the physical causes of negative resistance were not understood, engineers knew it could generate oscillations and had begun to apply it.[147] Heinrich Barkhausen in 1907 showed that oscillators must have negative resistance.[93] Ernst Ruhmer and Adolf Pieper discovered that mercury vapor lamps could produce oscillations, and by 1912 AT&T had used them to build amplifying repeaters for telephone lines.[147]

In 1918 Albert Hull at GE discovered that vacuum tubes could have negative resistance in parts of their operating ranges, due to a phenomenon called secondary emission.[155] In a vacuum tube when electrons strike the plate electrode they can knock additional electrons out of the surface into the tube. This represents a current away from the plate, reducing the plate current. Under certain conditions increasing the plate voltage causes a decrease in plate current. By connecting an LC circuit to the tube Hull created an oscillator, the dynatron oscillator. Other negative resistance tube oscillators followed, such as the magnetron (Hull, 1920).

The negative impedance converter originated from work by Marius Latour around 1920.[156][157] He was also one of the first to report negative capacitance and inductance.[156] Vacuum tube NICs were developed as telephone line repeaters at Bell Labs by George Crisson and others around 1931[47][134] and made transcontinental telephone service possible.[134] Transistor NICs, pioneered by Linnvill (1953), initiated a great increase in interest in NICs and many new circuits and applications developed.[131][134]

### Solid state devices

Negative differential resistance in semiconductors was observed around 1909 in the first point-contact junction diodes, called cat's whisker detectors, by researchers such as William Henry Eccles[158][159] and G. W. Pickard.[159][160][161] They noticed that when junctions were biased with a DC voltage to improve their sensitivity as radio detectors, they would sometimes break into spontaneous oscillations.[161] However the effect was not pursued.

The first person to exploit negative resistance diodes practically was Russian radio researcher Oleg Losev, who in 1922 discovered negative differential resistance in biased zincite (zinc oxide) point contact junctions.[161][162][163][164][165] He used these to build solid-state amplifiers, oscillators, and amplifying and regenerative radio receivers, 25 years before the invention of the transistor.[158][163][165][166] Later he even built a superheterodyne receiver.[165] However his achievements were overlooked because of the success of vacuum tube technology. After ten years he abandoned research into this technology (dubbed "Crystodyne" by Hugo Gernsback),[166] and it was forgotten.[165]

The first widely used solid-state negative resistance device was the tunnel diode, invented in 1957 by Japanese physicist Leo Esaki.[37] Because they have lower parasitic capacitance than vacuum tubes due to their small junction size, diodes can function at higher frequencies, and tunnel diode oscillators proved able to produce power at microwave frequencies, above the range of ordinary vacuum tube oscillators. Its invention set off a search for other negative resistance semiconductor devices for use as microwave oscillators,[167] resulting in the discovery of the IMPATT diode, Gunn diode, TRAPATT diode, and others. In 1969 Kurokawa derived conditions for stability in negative resistance circuits.[140] Currently negative differential resistance diode oscillators are the most widely used sources of microwave energy,[89] and many new negative resistance devices have been discovered in recent decades.[37]

## Notes

1. ^ a b c d The terms "open-circuit stable" and "short-circuit stable" have become somewhat confused over the years, and are used in the opposite sense by some authors. The reason is that in linear circuits if the load line crosses the I-V curve of the NR device at one point, the circuit is stable, while in nonlinear switching circuits that operate by hysteresis the same condition causes the circuit to become unstable and oscillate as an astable multivibrator, and the bistable region is considered the "stable" one. This article uses the former "linear" definition, the earliest one, which is that VCNRs are stable for $\scriptstyle R_L\;<\;r$, "short-circuit stable" and CCNRs are stable for $\scriptstyle R_L\;>\;r$, "open-circuit stable", found in the Abraham, Bangert, Dorf, Golio, and Tellegen sources. The latter "switching circuit" definition, which is that VCNRs are stable for $\scriptstyle R_L\;>\;r$, "open-circuit stable" and CCNRs are stable for $\scriptstyle R_L\;<\;r$, "closed-circuit stable", is found in the Kumar and Taub sources.

## References

1. Sinclair, Ian Robertson (2001). Sensors and transducers, 3rd Ed.. Newnes. pp. 69–70. ISBN 0750649321.
2. ^ a b Kularatna, Nihal (1998). Power Electronics Design Handbook. Newnes. pp. 232–233. ISBN 0750670738.
3. Aluf, Ofer (2012). Optoisolation Circuits: Nonlinearity Applications in Engineering. World Scientific. pp. 8–11. ISBN 9814317004. This source uses the term "absolute negative differential resistance" to refer to active resistance
4. ^ Institute of Electrical and Electronic Engineers (2000). IEEE 100: The Authoritative Dictionary of IEEE Standards Terms. IEEE Press. p. 732. ISBN 0738126012.
5. ^ Amos, Stanley William; Amos, Roger S.; Dummer, Geoffrey William Arnold (1999). Newnes Dictionary of Electronics, 4th Ed.. Newnes. p. 211. ISBN 0750643315.
6. Snelgrove, Martin (2008). "Negative resistance circuits". AccessScience Online Encyclopedia. McGraw-Hill. Retrieved May 17, 2012. on Answers.com website In this source active resistance is referred to as ideal negative resistance
7. ^ Graf, Rudolf F. (1999). Modern Dictionary of Electronics, 7th Ed.. Newnes. p. 499. ISBN 0750698667.
8. Shanefield, Daniel J. (2001). Industrial Electronics for Engineers, Chemists, and Technicians. Elsevier. pp. 18–19. ISBN 0815514670.
9. Carr, Joseph J. (1997). Microwave & Wireless Communications Technology. USA: Newnes. pp. 313–314. ISBN 0750697075.
10. Gottlieb, Irving M. (1997). Practical Oscillator Handbook. Elsevier. pp. 75–76. ISBN 0080539386.
11. Kaplan, Ross M. (December 1968). "Equivalent circuits for negative resistance devices". Technical Report No. RADC-TR-68-356. Rome Air Development Center, US Air Force Systems Command. pp. 5–8. Retrieved September 21, 2012.
12. "In semiconductor physics, it is known that if a two-terminal device shows negative differential resistance it can amplify." Suzuki, Yoshishige; Kuboda, Hitoshi (March 10, 2008). "Spin-torque diode effect and its application". Journal of the Physical Society of Japan (Tokyo: PSJ) 77 (3). doi:10.1143/JPSJ.77.031002. Retrieved June 13, 2013.
13. ^ a b c d Iniewski, Krzysztof (2007). Wireless Technologies: Circuits, Systems, and Devices. CRC Press. p. 488. ISBN 0849379962.
14. Horowitz, Paul; Winfield Hill (1989). The Art of Electronics, 2nd Ed.. UK: Cambridge University Press. pp. 14–15. ISBN 0521370957. The circuit shown in this source is slightly different in that the output is taken across the resistor $\scriptstyle R$ instead of the diode, but functions similarly.
15. ^ a b c d Shahinpoor, Mohsen; Schneider, Hans-Jörg (2008). Intelligent Materials. London: Royal Society of Chemistry. p. 209. ISBN 0854043357.
16. ^ a b c Golio, Mike (2000). The RF and Microwave Handbook. CRC Press. p. 5.91. ISBN 1420036769.
17. Kumar, Umesh (April 2000). "Design of an indiginized negative resistance characteristics curve tracer". Active and Passive Elect. Components (Hindawi Publishing Corp.) 23: 1–2. Retrieved May 3, 2013.
18. Beneking, H. (1994). High Speed Semiconductor Devices: Circuit aspects and fundamental behaviour. Springer. pp. 114–117. ISBN 0412562200.
19. Wilson, Marcus (November 16, 2010). "Negative Resistance". Sciblog 2010 Archive. Science Media Center. Retrieved September 26, 2012.
20. Simin, Grigory (2011). "Lecture 08: Tunnel Diodes (Esaki diode)". ELCT 569: Semiconductor Electronic Devices. Prof. Grigory Simin, Univ. of South Carolina. Retrieved September 25, 2012., pp. 18–19
21. Baker, R. Jacob (2011). CMOS: Circuit Design, Layout, and Simulation. John Wiley & Sons. p. 21.29. ISBN 1118038231. In this source "negative resistance" refers to negative static resistance.
22. Chua, Leon (2000). Linear and Non Linear Circuits. McGraw-Hill Education. pp. 49–50. ISBN 0071166505.
23. Gilmore, Rowan; Les Besser (2003). Active Circuits and Systems. USA: Artech House. pp. 27–29. ISBN 9781580535229.
24. Fogiel, Max (1988). The electronics problem solver. Research & Education Assoc. pp. 1032.B–1032.D. ISBN 0878915435.
25. Rybin, Yu. K. (2011). Electronic Devices for Analog Signal Processing. Springer. pp. 155–156. ISBN 9400722044.
26. ^ Iezekiel, Stavros (2008). Microwave Photonics: Devices and Applications. John Wiley and Sons. p. 120. ISBN 0470744863.
27. ^ a b c d Kapoor, Virender; S. Tatke (1999). Telecom Today: Application and Management of Information Technology. Allied Publishers. pp. 144–145. ISBN 8170239605.
28. ^ a b c Radmanesh, Matthew M. (2009). Advanced RF & Microwave Circuit Design. AuthorHouse. pp. 479–480. ISBN 1425972438.
29. ^ a b Whitaker, Jerry C. (2005). The electronics handbook, 2nd Ed.. CRC Press. p. 379. ISBN 0849318890.
30. ^ Gilmour, A. S. (2011). Klystrons, Traveling Wave Tubes, Magnetrons, Cross-Field Amplifiers, and Gyrotrons. Artech House. pp. 490–491. ISBN 1608071847.
31. ^ Illingworth, Valerie (2009). Astronomy. Infobase Publishing. p. 290. ISBN 1438109326.
32. ^ Rao, R. S. (2012). Microwave Engineering. PHI Learning Pvt. Ltd. p. 440. ISBN 8120345142.
33. ^ a b c Ayrton, Hertha (August 16, 1901). "The Mechanism of the Electric Arc". The Electrician (London: The Electrician Printing & Publishing Co.) 47 (17): 635–636. Retrieved January 2, 2013.
34. ^ Satyam, M.; K. Ramkumar (1990). Foundations of Electronic Devices. New Age International. p. 501. ISBN 8122402941.
35. Ghadiri, Aliakbar (Fall 2011). "Design of Active-Based Passive Components for Radio Frequency Applications". PhD Thesis. Electrical and Computer Engineering Dept., Univ. of Alberta. pp. 9–10. Retrieved March 21, 2014.
36. ^ a b c see "Negative resistance by means of feedback" section, Pippard, A. B. (2007). The Physics of Vibration. Cambridge University Press. pp. 314–326. ISBN 0521033330.
37. Franz, Roger L. (June 24, 2010). "Use nonlinear devices as linchpins to next-generation design". Electronic Design magazine (Penton Media Inc.). Retrieved September 17, 2012. An expanded version of this article with graphs and an extensive list of new negative resistance devices appears in Franz, Roger L. (2012). "Overview of Nonlinear Devices and Circuit Applications". Sustainable Technology. Roger L. Franz personal website. Retrieved September 17, 2012.
38. ^ a b Herrick, Robert J. (2003). DC/AC Circuits and Electronics: Principles & Applications. Cengage Learning. pp. 106, 110–111. ISBN 0766820831.
39. Horowitz, Paul; Winfield Hill (1989). The Art of Electronics, 2nd Ed.. Cambridge University Press. pp. 61, 64. ISBN 0521370957.
40. ^ a b c Webster, J., Ed. (1999). Wiley Encyclopedia of Electrical and Electronics Engineering. John Wiley & Sons. pp. 90–91. ISBN 0471139467. on [1]
41. ^ a b c Haisch, Bernhard (2013). "Nonlinear conduction". Online textbook Vol. 1: DC Circuits. All About Circuits website. Retrieved March 8, 2014.
42. Simpson, R. E. (1987). Introductory Electronics for Scientists and Engineers, 2nd Ed.. US: Addison-Wesley. pp. 4–5. ISBN 0205083773.
43. ^ a b c Nahvi, Mahmood; Joseph A Edminister (2004). Schaum's Easy Outline of Electric Circuits. McGraw-Hill Professional. pp. 14, 16. ISBN 0071422412.
44. Lesurf, Jim (2006). "Negative Resistance Oscillators". The Scots Guide to Electronics. School of Physics and Astronomy, Univ. of St. Andrews. Retrieved August 20, 2012.
45. ^ Forbes T. Brown (2006). Engineering System Dynamics. CRC Press. p. 43. ISBN 978-0-8493-9648-9.
46. ^ a b c Kaiser, Kenneth L. (2004). Electromagnetic Compatibility Handbook. CRC Press. pp. 13–52. ISBN 978-0-8493-2087-3.
47. Crisson, George (July 1931). "Negative Impedances and the Twin 21-Type Repeater". Bell System Tech. J. (USA: AT&T) 10 (3): 485–487. doi:10.1002/j.1538-7305.1931.tb01288.x. Retrieved December 4, 2012.
48. Morecroft, John Harold; A. Pinto; Walter Andrew Curry (1921). Principles of Radio Communication. US: John Wiley and Sons. p. 112.
49. ^ a b c d Reich, Herbert J. (1941). Principles of Electron Tubes. US: McGraw-Hill. p. 215. on Peter Millet's Tubebooks website
50. ^ a b c d Kouřil, František; Vrba, Kamil (1988). Non-linear and parametric circuits: principles, theory and applications. Ellis Horwood. p. 38. ISBN 0853126062.
51. Horowitz, Paul (2004). "Negative Resistor – Physics 123 demonstration with Paul Horowitz". Video lecture, Physics 123, Harvard Univ. YouTube. Retrieved November 20, 2012. In this video Prof. Horowitz demonstrates that negative static resistance actually exists. He has a black box with two terminals, labelled "−10 kilohms" and shows with ordinary test equipment that it acts like a linear negative resistor (active resistor) with a resistance of −10 KΩ: a positive voltage across it causes a proportional negative current through it, and when connected in a voltage divider with an ordinary resistor the output of the divider is greater than the input, it can amplify. At the end he opens the box and shows it contains an op-amp negative impedance converter circuit and battery.
52. "...since [static] resistance is always positive...the resultant power [from Joule's law] must also always be positive. ...[this] means that the resistor always absorbs power." Karady, George G.; Holbert, Keith E. (2013). Electrical Energy Conversion and Transport: An Interactive Computer-Based Approach, 2nd Ed.. John Wiley and Sons. p. 3.21. ISBN 1118498038.
53. ^ a b c "Since the energy absorbed by a (static) resistance is always positive, resistances are passive devices." Bakshi, U.A.; V.U.Bakshi (2009). Electrical And Electronics Engineering. Technical Publications. p. 1.12. ISBN 8184316976.
54. ^ a b c Glisson, Tildon H. (2011). Introduction to Circuit Analysis and Design. USA: Springer. pp. 114–116. ISBN 9048194423., see footnote p. 116
55. ^ a b c d Traylor, Roger L. (2008). "Calculating Power Dissipation". Lecture Notes – ECE112:Circuit Theory. Dept. of Elect. and Computer Eng., Oregon State Univ. Retrieved 23 October 2012.
56. Hoekstra, Jaap (2010). Introduction to Nanoelectronic Single-Electron Circuit Design. USA: Pan Stanford Publishing. p. 131. ISBN 9814241938.
57. ^ a b Laplante, Philip A. (2005). Comprehensive Dictionary of Electrical Engineering, 2nd Ed.. CRC Press. p. 465. ISBN 1420037803.
58. Dimopoulos, Hercules G. (2011). Analog Electronic Filters: Theory, Design and Synthesis. Springer. pp. 372–374. ISBN 9400721897.
59. ^ a b c Pippard, A. B. (2007). The Physics of Vibration. Cambridge University Press. pp. 350, fig. 36; p. 351, fig. 37a; p. 352 fig. 38c; p. 327, fig. 14c. ISBN 0521033330. In some of these graphs, the curve is reflected in the vertical axis so the negative resistance region appears to have positive slope.
60. Butler, Lloyd (November 1995). "Negative Resistance Revisited". Amateur Radio magazine. Wireless Institute of Australia Bayswater, Victoria. Retrieved September 22, 2012. on Lloyd Butler's personal website
61. ^ a b c Razavi, Behzad (2001). Design of Analog CMOS Integrated Circuits. The McGraw-Hill Companies. pp. 505–506. ISBN 7302108862.
62. Solymar, Laszlo; Donald Walsh (2009). Electrical Properties of Materials, 8th Ed.. UK: Oxford University Press. pp. 181–182. ISBN 0199565910.
63. ^ a b c Prasad, Sheila; Hermann Schumacher; Anand Gopinath (2009). High-Speed Electronics and Optoelectronics: Devices and Circuits. Cambridge Univ. Press. p. 388. ISBN 0521862833.
64. Deliyannis, T.; Yichuang Sun, J.K. Fidler (1998). Continuous-Time Active Filter Design. CRC Press. pp. 82–84. ISBN 0849325730.
65. Hickman, Ian (1999). Analog Circuits Cookbook, 2nd Ed.. New York: Newnes. pp. 4–6, 28. ISBN 0750642343.
66. ^ a b Popa, Cosmin Radu (2012). Synthesis of Analog Structures for Computational Signal Processing. Springer. p. 323. ISBN 978-1-4614-0403-3.
67. ^ a b c Miano, Giovanni; Antonio Maffucci (2001). Transmission Lines and Lumped Circuits. Academic Press. pp. 396, 397. ISBN 0121897109. This source calls negative differential resistances "passive resistors" and negative static resistances "active resistors".
68. ^ a b Fett, G. H. (October 4, 1943). "Negative Resistance as a Machine Parameter". Journal of Applied Physics (American Institute of Physics) 14 (12): 674–678. doi:10.1063/1.1714945. Retrieved December 2, 2012., abstract.
69. ^ Combatti, Matt (November 25, 2011). "Negative Resistor – Ion Bottle". Articles. Let's Replicate website. Retrieved December 3, 2012.
70. ^ John, Bedini (2002). "Welcome to Bedini Technology". John Bedini personal website. Retrieved December 3, 2012.
71. ^ Bearden, Tom (April 27, 2000). "Breakthrough – Bedini's Brilliant Formation Of Negative Resistors In Batteries". Rense.com. Jeff Rense personal website. Retrieved December 3, 2012.
72. ^ Craddock, Anthony J. (2001). "Gabriel Kron and the Negative Resistor". A Summary Review of Energy and Antigravity Research. Disclosure Project – Briefing Document. Retrieved December 3, 2012. on BibliotecaPleyades.com website
73. ^ Bearden, T. E. (June 6, 2000). "Giant negentropy from the common dipole". Exploring Free Energy, Gravity/Antigravity, and Time. Intalek, Inc. William Alek's personal website. Retrieved December 3, 2012.
74. ^ Puhl, Marcelo (April 7, 2000). "The Negistor & Negative Resistance". Exploring Free Energy, Gravity/Antigravity, and Time. Intalek, Inc. William Alek's personal website. Retrieved December 3, 2012.
75. Thompson, Sylvanus P. (July 3, 1896). "On the properties of a body having a negative electric resistance". The Electrician (London: Benn Bros.) 37 (10): 316–318. Retrieved June 7, 2014. also see editorial, "Positive evidence and negative resistance", p. 312
76. ^ a b Grant, Paul M. (July 17, 1998). "Journey Down the Path of Least Resistance" (PDF). OutPost on the Endless Frontier blog. EPRI News, Electric Power Research Institute. Retrieved December 8, 2012. on Paul Grant personal website
77. ^ Cole, K.C. (July 10, 1998). "Experts Scoff at Claim of Electricity Flowing With 'Negative Resistance'". Los Angeles Times (Los Angeles: Tribune Co.). Retrieved December 8, 2012. on Los Angeles Times website. In this article the term "negative resistance" refers to negative static resistance.
78. ^ a b Klein, Sanford; Gregory Nellis (2011). Thermodynamics. Cambridge University Press. p. 206. ISBN 1139498185.
79. ^ resonant.freq (November 2, 2011). "Confusion regarding negative resistance circuits". Electrical Engineering forum. Physics Forums, Arizona State Univ. Retrieved August 17, 2014.
80. ^ a b Gibilisco, Stan (2002). Physics Demystified. McGraw Hill Professional. p. 391. doi:10.1036/0071412123. ISBN 0071412123.
81. ^ How electrical and electronic engineers use Ohm's law. Physics Quick Study Guide for Smartphones and Mobile Devices (MobileReference). 2007. ISBN 1605010715. Retrieved 4 December 2013.
82. ^ a b c Chen, Wai-Kai (2006). Nonlinear and distributed circuits. CRC Press. pp. 1.18–1.19. ISBN 0849372763.
83. ^ a b see Chua, Leon O. (November 1980). "Dynamic Nonlinear Networks: State of the Art". IEEE Trans. on Circuits and Systems (US: Inst. of Electrical and Electronic Engineers). CAS-27 (11): 1076–1077. Retrieved September 17, 2012. Definitions 6 & 7, fig. 27, and Theorem 10 for precise definitions of what this condition means for the circuit solution.
84. ^ a b Muthuswamy, Bharathwaj; Joerg Mossbrucker (2010). "2010 Conference Proceedings". American Society for Engineering Education. Retrieved October 18, 2012. |chapter= ignored (help), Appendix B. This derives a slightly more complicated circuit where the two voltage divider resistors are different to allow scaling, but it reduces to the text circuit by setting R2 and R3 in the source to R1 in the text, and R1 in source to Z in the text. The I–V curve is the same.
85. Kumar, Anand (2004). Pulse and Digital Circuits. PHI Learning Pvt. Ltd. pp. 274, 283–289. ISBN 8120325966.
86. ^ among the first to distinguish the different types of negative resistance was Herold, Edward W. (October 1935). "Negative resistance and devices for obtaining it". Proc. of the IRE (Institute of Radio Engineers (now IEEE)) 23 (10): 1201–1223. doi:10.1109/JRPROC.1935.227271. ISSN 0731-5996. Retrieved July 30, 2013.
87. ^ a b c d Tellegen, B. d. h. (April 1972). "Stability of negative resistances". International Journal of Electronics (Taylor & Frances) 32 (6): 681–686. doi:10.1080/00207217208938331. Retrieved September 21, 2012.
88. ^ Kidner, C.; I. Mehdi; J. R. East; J. I. Haddad (March 1990). "First International Symposium on Space Terahertz Technology, March 5–6, 1990, Univ. of Michigan". Ann Arbor, M: US National Radio Astronomy Observatory. p. 85. Retrieved October 17, 2012. |chapter= ignored (help)
89. ^ a b c d Du, Ke-Lin; M. N. S. Swamy (2010). Wireless Communication Systems: From RF Subsystems to 4G Enabling Technologies. Cambridge Univ. Press. p. 438. ISBN 0521114039.
90. ^ a b c Abraham, George (1974). "Advances in Electronics and Electron Physics, Vol. 34–35". Academic Press. pp. 270–398. Retrieved September 17, 2012. |chapter= ignored (help)
91. ^ a b c Weaver, Robert (2009). "Negative Resistance Devices: Graphical Analysis and Load Lines". Bob's Electron Bunker. Robert Weaver personal website. Retrieved December 4, 2012.
92. ^ a b Lowry, H. R.; J. Georgis; E. Gottlieb (1961). General Electric Tunnel Diode Manual, 1st Ed.. New York: General Electric Corp. pp. 18–19.
93. ^ a b c d The requirements for negative resistance in oscillators, "For alternating current power to be available in a circuit which has externally applied only continuous voltages, the average power consumption during a cycle must be negative...which demands the introduction of negative resistance [which] requires that the phase difference between voltage and current lie between 90° and 270°...[and for nonreactive circuits] the value 180° must hold... The volt-ampere characteristic of such a resistance will therefore be linear, with a negative slope..." were first set forth by Heinrich Barkhausen in 1907 in Das Problem Der Schwingungserzeugung according to Duncan, R. D. (March 1921). "Stability conditions in vacuum tube circuits". Physical Review (American Physical Society) 17 (3): 304. doi:10.1103/physrev.17.302. Retrieved July 17, 2013.
94. Frank, Brian (2006). "Microwave Oscillators" (PDF). Class Notes:ELEC 483 – Microwave and RF Circuits and Systems. Dept. of Elec. and Computer Eng., Queen's Univ., Ontario. pp. 4–9. Retrieved September 22, 2012.
95. Golio (2000) The RF and Microwave Handbook, pp. 7.25–7.26, 7.29
96. ^ a b Chang, Kai (2000). RF and Microwave Wireless Systems. USA: John Wiley & Sons. pp. 139–140. ISBN 0471351997.
97. Maas, Stephen A. (2003). Nonlinear Microwave and RF Circuits, 2nd Ed.. Artech House. pp. 542–544. ISBN 1580534848.
98. ^ Mazda, F. F. (1981). Discrete Electronic Components. CUP Archive. p. 8. ISBN 0521234700.
99. ^ Bowick, Chris Bowick; John Blyler; Cheryl J. Ajluni (2008). RF Circuit Design, 2nd Ed.. USA: Newnes. p. 111. ISBN 0750685182.
100. ^ a b Rhea, Randall W. (2010). Discrete Oscillator Design: Linear, Nonlinear, Transient, and Noise Domains. USA: Artech House. pp. 57, 59. ISBN 1608070476.
101. ^ Chen, Wai Kai (2004). The Electrical Engineering Handbook. Academic Press. pp. 80–81. ISBN 0080477488.
102. ^ Dorf, Richard C. (1997). The Electrical Engineering Handbook (2 ed.). CRC Press. p. 179. ISBN 1420049763.
103. ^ Vukic, Zoran (2003). Nonlinear Control Systems. CRC Press. pp. 53–54. ISBN 0203912659.
104. ^ a b c Crisson (1931) Negative Impedances and the Twin 21-Type Repeater, pp. 488–492
105. ^ a b c Karp, M. A. (May 1956). "A transistor D-C negative immittance converter". APL/JHU CF-2524. Advanced Physics Lab, Johns Hopkins Univ. pp. 3, 25–27. Retrieved December 3, 2012. on US Defense Technical Information Center website
106. ^ a b Giannini, Franco; Leuzzi, Giorgio (2004). Non-linear Microwave Circuit Design. John Wiley and Sons. pp. 230–233. ISBN 0470847018.
107. ^ a b Yngvesson, Sigfrid (1991). Microwave Semiconductor Devices. Springer Science & Business Media. p. 143. ISBN 079239156X.
108. ^ a b Bangert, J. T. (March 1954). "The Transistor as a Network Element". Bell System Tech. J. (USA: American Tel. and Tel.) 33 (2): 330. Retrieved June 20, 2014.
109. ^ Gilmore, Rowan; Besser, Les (2003). Practical RF Circuit Design for Modern Wireless Systems 2. Artech House. pp. 209–214. ISBN 1580536743.
110. ^ a b c d Krugman, Leonard M. (1954). Fundamentals of Transistors. New York: John F. Rider. pp. 101–102. reprinted on Virtual Institute of Applied Science website
111. ^ a b c d Gottlieb 1997 Practical Oscillator Handbook, pp. 105–108
112. Nahin, Paul J. (2001). The Science of Radio: With Matlab and Electronics Workbench Demonstration, 2nd Ed.. Springer. pp. 81–85. ISBN 0387951504.
113. ^ a b Spangenberg, Karl R. (1948). Vacuum Tubes. McGraw-Hill. p. 721., fig. 20.20
114. ^ a b c Armstrong, Edwin H. (August 1922). "Some recent developments of regenerative circuits". Proc. of the Inst. of Radio Engineers (New York: Institute of Radio Engineers) 10 (4): 244–245. doi:10.1109/jrproc.1922.219822. Retrieved September 9, 2013.. "Regeneration" means "positive feedback"
115. ^ a b Technical Manual no. 11-685: Fundamentals of Single-Sideband Communication. US Dept. of the Army and Dept. of the Navy. 1961. p. 93.
116. ^ Singh, Balwinder; Dixit, Ashish (2007). Analog Electronics. Firewall Media. p. 143. ISBN 8131802450.
117. ^ Pippard, A. B. (1985). Response and stability: an introduction to the physical theory. CUP Archive. pp. 11–12. ISBN 0521266734. This source uses "negative resistance" to mean active resistance
118. ^ Podell, A.F.; Cristal, E.G. (May 1971). "Microwave Symposium Digest, 1971 IEEE GMTT International 16–19 May 1971". USA: Institute of Electrical and Electronic Engineers. pp. Abstract. Retrieved December 19, 2012. |chapter= ignored (help) on IEEE website
119. ^ Simons, Elliot (March 18, 2002). "Consider the "Deboo" integrator for unipolar noninverting designs". Electronic Design magazine website. Penton Media, Inc. Retrieved November 20, 2012.
120. ^ Hamilton, Scott (2007). An Analog Electronics Companion: Basic Circuit Design for Engineers and Scientists. Cambridge University Press. p. 528. ISBN 0521687802.
121. ^ a b this property was often called "resistance neutralization" in the days of vacuum tubes, see Bennett, Edward; Leo James Peters (January 1921). "Resistance Neutralization: An application of thermionic amplifier circuits". Jour. of the AIEE (New York: American Institute of Electrical Engineers) 41 (1): 234–248. Retrieved August 14, 2013. and Ch. 3: "Resistance Neutralization" in Peters, Leo James (1927). Theory of Thermionic Vacuum Tube Circuits. McGraw-Hill. pp. 62–87.
122. Lee, Thomas H. (2004). The Design of CMOS Radio-Frequency Integrated Circuits, 2nd Ed.. UK: Cambridge University Press. pp. 641–642. ISBN 0521835399.
123. Kung, Fabian Wai Lee (2009). "Lesson 9: Oscillator Design" (PDF). RF/Microwave Circuit Design. Prof. Kung's website, Multimedia University. Retrieved October 17, 2012., Sec. 3 Negative Resistance Ocillators, pp. 9–10, 14
124. Räisänen, Antti V.; Arto Lehto (2003). Radio Engineering for Wireless Communication and Sensor Applications. USA: Artech House. pp. 180–182. ISBN 1580535429.
125. Ellinger, Frank (2008). Radio Frequency Integrated Circuits and Technologies, 2nd Ed.. USA: Springer. pp. 391–394. ISBN 3540693246.
126. ^ a b Li, Dandan; Yannis Tsividis (2002). "Design of High Frequency Integrated Analogue Filters". Institution of Engineering and Technology (IET). p. 58. ISBN 0852969767. Retrieved July 23, 2013. |chapter= ignored (help)
127. ^ a b Rembovsky, Anatoly (2009). Radio Monitoring: Problems, Methods and Equipment. Springer. p. 24. ISBN 0387981004.
128. ^ a b c Sun, Yichuang Sun (2002). Design of High Frequency Integrated Analogue Filters. IET. pp. 58, 60–62. ISBN 0852969767.
129. ^ Carr, Joseph (2001). Antenna Toolkit, 2nd Ed.. Newnes. p. 193. ISBN 0080493882.
130. ^ a b c Kennedy, Michael Peter (October 1993). "Three Steps to Chaos: Part 1 – Evolution". IEEE Trans. on Circuits and Systems (Inst. of Electrical and Electronic Engineers) 40 (10): 640. doi:10.1109/81.246140. Retrieved February 26, 2014.
131. ^ a b Linvill, J.G. (1953). "Transistor Negative-Impedance Converters". Proceedings of the IRE 41 (6): 725–729. doi:10.1109/JRPROC.1953.274251.
132. Horowitz (1989) The Art of Electronics, 2nd Ed., pp. 266–267
133. ^ "Application Note 1868: Negative resistor cancels op-amp load". Application Notes. Maxim Integrated, Inc. website. January 31, 2003. Retrieved October 8, 2014.
134. ^ a b c d Hansen, Robert C.; Robert E. Collin (2011). Small Antenna Handbook. John Wiley & Sons. pp. sec. 2–6, pp. 262–263. ISBN 0470890835.
135. ^ a b Aberle, James T.; Robert Loepsinger-Romak (2007). Antennas With Non-Foster Matching Networks. Morgan & Claypool. pp. 1–8. ISBN 1598291025.
136. ^ a b Haddad, G. I.; J. R. East; H. Eisele (2003). "Terahertz Sensing Technology: Electronic devices and advanced systems technology". World Scientific. p. 45. Retrieved October 17, 2012. |chapter= ignored (help)
137. ^ Horowitz, 1989, p. 285
138. ^ a b Kung, Fabian Wai Lee (2009). "Lesson 9: Oscillator Design" (PDF). RF/Microwave Circuit Design. Prof. Kung's website, Multimedia University. Retrieved October 17, 2012., Sec. 3 Negative Resistance Ocillators, p. 21
139. ^ Kshetrimayum, Rakhesh Singh. "Experiment 5: Study of I–V Characteristics of Gunn Diodes" (PDF). EC 341 Microwave Laboratory. Electrical Engineering Dept., Indian Institute of Technology, Guwahati, India. Retrieved January 8, 2013.
140. ^ a b c Kurokawa, K. (July 1969). "Some Basic Characteristics of Broadband Negative Resistance Oscillator Circuits". Bell System Tech. J. (USA: American Tel. & Tel.) 48 (6): 1937–1955. doi:10.1002/j.1538-7305.1969.tb01158.x. Retrieved December 8, 2012. Eq. 10 is the necessary condition for oscillation, eq. 12 is sufficient condition.
141. ^ a b c d Rohde, Ulrich L.; Ajay K. Poddar; Georg Böck (2005). The Design of Modern Microwave Oscillators for Wireless Applications:Theory and Optimization. USA: John Wiley & Sons. pp. 96–97. ISBN 0471727164.
142. ^ a b Das, Annapurna; Das, Sisir K. (2000). Microwave Engineering. Tata McGraw-Hill Education. pp. 394–395. ISBN 0074635778.
143. ^ a b H. C. Okean, Tunnel diodes in Willardson, Robert K.; Beer, Albert C., Eds. (1971). Semiconductors and Semimetals, Vol. 7 Part B. Academic Press. pp. 546–548. ISBN 0080863973.
144. Chang, Kai, Millimeter-wave Planar Circuits and Subsystems in Button, Kenneth J., Ed. (1985). Infrared and Millimeter Waves: Millimeter Components and Techniques, Part 5 14. Academic Press. pp. 133–135. ISBN 0323150616.
145. ^ a b c Linkhart, Douglas K. (2014). Microwave Circulator Design (2 ed.). Artech House. pp. 78–81. ISBN 1608075834.
146. ^ MacLean, Jason N.; Schmidt, Brian J. (September 2001). "Voltage-Sensitivity of Motoneuron NMDA Receptor Channels Is Modulated by Serotonin in the Neonatal Rat Spinal Cord". Jour. of Neurophysiology (American Physiological Society) 86 (3): 1131–1138. Retrieved August 18, 2014.
147. Hong, Sungook (2001). Wireless: From Marconi's Black-Box to the Audion. USA: MIT Press. pp. 159–165. ISBN 0262082985.
148. ^ A. Niaudet, La Lumiere Electrique, No. 3, 1881, p. 287, cited in Encyclopaedia Britannica, 11th Ed., Vol. 16, p. 660
149. ^ a b c d Emile Garcke, "Lighting". Encyclopaedia Britannica, 11th Ed 16. The Encyclopaedia Britannica Co. 1911. pp. 660–661. Retrieved 2012-04-11.
150. ^ Heaviside, Oliver (July 31, 1892). "Correspondence: Negative Resistance". The Electrician (London: "The Electrician" Printing and Publishing Co.) 37 (14): 452. Retrieved December 24, 2012., also see letter by Andrew Gray on same page
151. Gethemann, Daniel (2012). "Singing Arc: The Usefulness of Negative Resistance". Zauberhafte Klangmaschinen. Institut fur Medienarchaologie. Retrieved 2012-04-11.
152. ^ Frith, Julius; Charles Rodgers (November 1896). "On the Resistance of the Electric Arc". London, Edinburgh, and Dublin Philosophical Magazine (London: Taylor and Francis) 42 (258): 407–423. doi:10.1080/14786449608620933. Retrieved May 3, 2013.
153. ^ G. Fitzgerald, On the Driving of Electromagnetic Vibrations by Electromagnetic and Electrostatic Engines, read at the January 22, 1892 meeting of the Physical Society of London, in Larmor, Joseph, Ed. (1902). The Scientific Writings of the late George Francis Fitzgerald. London: Longmans, Green and Co. pp. 277–281.
154. ^ Morse, A. H. (1925). Radio: Beam and Broadcast. London: Ernest Benn. p. 28.
155. ^ Hull, Albert W. (February 1918). "The Dynatron – A vacuum tube possessing negative electric resistance". Proceedings of the IRE (New York: Institute of Radio Engineers) 6 (1): 5–35. doi:10.1109/jrproc.1918.217353. Retrieved 2012-05-06.
156. ^ a b Latour, Marius (October 30, 1920). "Basic Theory of Electron-Tube Amplifiers – Part II". Electrical World (New York: McGraw-Hill) 76 (18): 870–872. Retrieved December 27, 2012.
157. ^ Merrill, J.L., Jr. (January 1951). "Theory of the Negative Impedance Converter". Bell System Tech. J. (USA: American Tel. & Tel.) 30 (1): 88–109. doi:10.1002/j.1538-7305.1951.tb01368.x. Retrieved December 9, 2012.
158. ^ a b Grebennikov, Andrei (2011). RF and Microwave Transmitter Design. John Wiley & Sons. p. 4. ISBN 047052099X.
159. ^ a b Pickard, Greenleaf W. (January 1925). "The Discovery of the Oscillating Crystal". Radio News (New York: Experimenter Publishing Co.) 6 (7): 1166. Retrieved July 15, 2014.
160. ^ "Strays". QST magazine (USA: American Radio Relay League) 6: 44. March 1920. Retrieved April 5, 2013.
161. ^ a b c White, Thomas H. (2003). "Section 14 – Expanded Audio and Vacuum Tube Development (1917–1924)". United States Early Radio History. earlyradiohistory.us. Retrieved September 23, 2012.
162. ^ Losev, O. V. (January 1925). "Oscillating Crystals". Radio News (New York: Experimenter Publishing Co.) 6 (7): 1167, 1287. Retrieved July 15, 2014.
163. ^ a b Gabel, Victor (October 1, 1924). "The Crystal as a Generator and Amplifier". The Wireless World and Radio Review (London: Iliffe & Sons Ltd.) 15: 2–5. Retrieved March 20, 2014.
164. ^ Ben-Menahem, Ari (2009). Historical Encyclopedia of Natural and Mathematical Sciences, Vol. 1. Springer. p. 3588. ISBN 3540688315.
165. ^ a b c d Lee, Thomas H. (2004) The Design of CMOS Radio-Frequency Integrated Circuits, 2nd Ed., p. 20
166. ^ a b Gernsback, Hugo (Sep 1924). "A Sensational Radio Invention". Radio News (Experimenter Publishing): 291. Retrieved May 23, 2012. and "The Crystodyne Principle", pp. 294–295
167. ^ Ridley, B. K. (May 7, 1964). ""Electric bubbles" and the quest for negative resistance". New Scientist (London: Cromwell House) 22 (390): 352–355. Retrieved November 15, 2012.