User:Ernstblumberg/sandbox

1699 OR EBX, PE_ 1700 1701 , RAM_START - size (STARTUP-DATA) 1702 MOV EAX, RAM_START 1703 ADD EAX, OFFSET (end_data) 1704 MOV EBX, RAM_START 1705 MOV ECX, CS_BASE 1706 ADD ECX, OFFSET (GDT_EPROM) 1707 1708 1709 1710 MOV APP_GDT_ram [EBX].table_lim, CX 1711 INC ECX 1712 MOVEDX, EAX 1713 MOV APP_GDT_ram[EBX].table_linear , EAX 1714 ADD EAX,ECX 1715 REP MOVS BYTE PTRES: [EDI],BYTE PTR DS :[ESI] 1716 1717 1717 1719 1720

1699 OR EBX, PE_ 1700 1701 , RAM_START - size (STARTUP-DATA) 1702 MOV EAX, RAM_START 1703 ADD EAX, OFFSET (end_data) 1704 MOV EBX, RAM_START 1705 MOV ECX, CS_BASE 1706 ADD ECX, OFFSET (GDT_EPROM) 1707 1708 1709 1710 MOV APP_GDT_ram [EBX].table_lim, CX 1711 INC ECX 1712 MOVEDX, EAX 1713 MOV APP_GDT_ram[EBX].table_linear , EAX 1714 ADD EAX,ECX 1715 REP MOVS BYTE PTRES: [EDI],BYTE PTR DS :[ESI] 1716 1717 1718 1719 1720

=Enc Prot SHA

BOOL EXPORTENCRYPTED: KEY = CxSshKey_CREATE ():)

// numbits may range from384 to 4096. TYPICAL VALUES ARE // 1024 OR 2048. (must be a multiple of 64 // A GOOD CHOICE FOR THE EXPONENT IS 65537. CHILKAT RECOMMENDS // ALWAYS USING THIS VALUE.

                          // NUMBITS = 2048; 
                          // EXPONENT = 65537;
                          // SUCCESS = CxSshKey; GeneratesRsaKey (key, numbits, exponent); 
                          // IF (SUCCESS ! = TRUE)
                                                                                        { PRINTP ("BAD params passed to RSA key generates method D"); RETURN;}
                          // NOTE: Generating a public/private key pair is CPU intensive
                          // and may take a short amount of time ' (more than a few seconds but less than a minute)

Ca2SupClXORcombinations(Raman/Zener)

M= 6.6 x 10^ - 26 kg p = h/(397nm) = 1.7 x 10^ -27 kgm/s <n> = (gamma/v_2)^2 = 0.01 Raman 1 = w_0-w_z transition|down n=0>---|up, n=1> Raman 2=transition|up, n=1>---|down, n=1> simultaneous 2π pulse transition|up, n=0>---|down, n=0>.

hya

beta peg,23h04'+24deg 05' NGC6383, M6: 17h40', -32deg12'

Recoil Frequencies

Recoil frequency = 120 kiloherz. Therefore use 100 micro second pulses. Optically push population to n=0 given that the laser is calibrated with a vibrational Quantum number n to n-1 for excited transitions. External magnetic field is approximately 100 Gauss (0.01 tesla). Rabi frequency is Ri R2/Delta when Rabi frequencies for S-P transitions are driven by each laser.

New Weapons Systems

Medical over ride: RJH - PEN

New weapons systems development Cobalt Niobate experiments are now clear and confirm Zamolodchikov calculations are correct and the magnetic perturbation has been confirmed - ramifications apply brillouin light shift equals very high acoustic frequencies cumulative E8 triality matrix arbitrary to rotate fermion generations solved and covariant vector fields are predictable and stable. PF weaponry 100 % and results to follow using system tray fire is green, orange is prepare to fire and blue is system wide broadcast commands use PFC software version when altering pulse current voltage and fault commands watch your Ping/System Status background counter.

Notes (SC PFG)

Kazhdan Lusztig Vogan computation of polynomials killing form signature -248 subgroup of GL248(R) in the ferromagnetic regime (gx<1) weak couplings between the magnetic chains are responsible for an effective magnetic field within a squid detector relative for angular velocities contours designated by S for enclosed areas. Bulk Superconductor n=0 so that Φ=n(φ)0+2m*/q*Ω.S magnetic fields and currents rotate at angular frequency Ω. Josephson Junctions functions as voltage controlled oscillator to generate very high frequencies (500 Ghz at 1mV). Josephson frequency applicable as v/V= Ω/2π=1/Ω0 ≡ 483.597898(19) Mhz/μV.

Reactive parallel jamming system US 7728755 B1 a control module for receiving data from receiving transmitting module and adapted to scan from data an operational spectrum and identify a signal as a potential threat based on signal exceeding threshold, etc. Incorporate implementation of piggy back signalling when hijacking systems and adapt full spectrum analyzers – Tektronix should suffice with logic analysis architecture.

G effective = g(1- (v/c)2). Allow for Lyapunov exponent the positive exponent λ+ is still 0.16 this will give the prediction time with the fractal dimension at 1.3 use magnetometer for ac Josephson effect junction required for stochaistic predictions. Plasma field is susceptible to to anomalous fluctuations. Magnetic field functions in parallel and all perturbations are anticipated and counter balanced classic superconductivity models apply within conventional nonlinearity parameters.

Instruction information – The precision of this resonant phenomenon is remarkable such that a frequency change of only 1:10,000,000,000 would prevent the atom absorbing the light. In this case the light is blue and has a frequency of 800,000,000,000,000 oscillations per second. When we are using the laser(s) this is essentially (together) with the quasi imperceptible diameter the reason for the extremities of super cooling. Regarding Joules we can be looking at 10n-28 in the lab+.

See Yadin 2008 output matrix C will be referred to as indices required result is C = Σ N- P/p=1 Σ M-Q/q=1 Cp,q = Σ N- P/p=1 Σ M-Q/q=1 Cp,q = →V p,q. (→Vp,q) use as a serial algorithm for computation C being Hermitian. Minimum variance method for synthetic aperture radar at – ignore the DRAM and plug in straight into the Hypercore and template using a variant of: foreach unique multiplication

m in the combination of :
val , A(r1,c1).A(r2,c2).
		Compute initial value of m. 

Foreach valid shift, (r^,c^), of m: Cr^,c^ ← Cr^,c^ + val

end

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