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::"Angular momentum or 3rd order sub particles are omitted as spin(2)=0,45,45."
::"Angular momentum or 3rd order sub particles are omitted as spin(2)=0,45,45."
–[[User:LaundryPizza03|'''<font color=#7f7fbf>Laundry</font><font color=#ffbf00>Pizza</font><font color=#bf0000>03</font>''']] ([[User talk:LaundryPizza03|<font color=#00df00>d</font>]][[Special:Contributions/LaundryPizza03|<font color=#00bfff>c&#x0304;</font>]]) 02:32, 11 May 2018 (UTC)
–[[User:LaundryPizza03|'''<font color=#7f7fbf>Laundry</font><font color=#ffbf00>Pizza</font><font color=#bf0000>03</font>''']] ([[User talk:LaundryPizza03|<font color=#00df00>d</font>]][[Special:Contributions/LaundryPizza03|<font color=#00bfff>c&#x0304;</font>]]) 02:32, 11 May 2018 (UTC)

== "Iso's" button associated with germanium does not function. ==

I tried the "Iso's" button for many other elements, and they work correctly. [[Special:Contributions/71.8.174.161|71.8.174.161]] ([[User talk:71.8.174.161|talk]]) 20:14, 2 October 2019 (UTC)

Revision as of 20:14, 2 October 2019

WikiProject iconElements: Isotopes List‑class Low‑importance
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This article is part of Wikipedia:Wikiproject Isotopes. Please keep style and phrasings consistent across the set of pages. For later reference and improved reliability, data from all considered multiple sources is collected here. References are denoted by these letters:

  • (A) G. Audi, O. Bersillon, J. Blachot, A.H. Wapstra. The Nubase2003 evaluation of nuclear and decay properties, Nuc. Phys. A 729, pp. 3-128 (2003). — Where this source indicates a speculative value, the # mark is also applied to values with weak assignment arguments from other sources, if grouped together. An asterisk after the A means that a comment of some importance may be available in the original.
  • (B) National Nuclear Data Center, Brookhaven National Laboratory, information extracted from the NuDat 2.1 database. (Retrieved Sept. 2005, from the code of the popup boxes).
  • (C) David R. Lide (ed.), Norman E. Holden in CRC Handbook of Chemistry and Physics, 85th Edition, online version. CRC Press. Boca Raton, Florida (2005). Section 11, Table of the Isotopes. — The CRC uses rounded numbers with implied uncertainties, where this concurs with the range of another source it is treated as exactly equal in this comparison.
  • (D) More specific level data from reference B's Levels and Gammas database.
  • (E) Same as B but excitation energy replaced with that from D.
  Z   N refs symbol   half-life                   spin              excitation energy
 32  26 AB  |Ge-58   |                           |0+
 32  27 A   |Ge-59   |                           |7/2-#
 32  28 A   |Ge-60   |30# ms                     |0+
 32  28 B   |Ge-60   |~30 ms                     |0+
 32  29 AB  |Ge-61   |39(12) ms                  |(3/2-)#
 32  29 C   |Ge-61   |0.04 s                     |
 32  30 A*  |Ge-62   |130(40) ms                 |0+
 32  30 B   |Ge-62   |129(35) ns                 |0+
 32  30 C   |Ge-62   |0.13 s                     |
 32  31 AB  |Ge-63   |142(8) ms                  |(3/2-)#
 32  31 C   |Ge-63   |0.15 s                     |
 32  32 ABC |Ge-64   |63.7(25) s                 |0+
 32  33 AB  |Ge-65   |30.9(5) s                  |(3/2)-
 32  33 C   |Ge-65   |31. s                      |
 32  34 AB  |Ge-66   |2.26(5) h                  |0+
 32  34 C   |Ge-66   |2.26 h                     |0+
 32  35 AB  |Ge-67   |18.9(3) min                |1/2-
 32  35 C   |Ge-67   |19.0 min                   |1/2-
 32  35 AD  |Ge-67m1 |13.7(9) µs                 |5/2-             |18.20(5) keV
 32  35 A   |Ge-67m2 |110.9(14) ns               |                 |751.70(6) keV
 32  35 D   |Ge-67m2 |110.9(14) ns               |9/2+             |751.70(6) keV
 32  36 AB  |Ge-68   |270.95(16) d               |0+
 32  36 C   |Ge-68   |270.8 d                    |0+
 32  37 ABC |Ge-69   |39.05(10) h                |5/2-
 32  37 AD  |Ge-69m1 |5.1(2) µs                  |1/2-             |86.765(14) keV
 32  37 AD  |Ge-69m2 |2.81(5) µs                 |9/2+             |397.944(18) keV
 32  38 ABC |Ge-70   |STABLE                     |0+
 32  39 AB  |Ge-71   |11.43(3) d                 |1/2-
 32  39 C   |Ge-71   |11.2 d                     |1/2-
 32  39 AD  |Ge-71m  |20.40(17) ms               |9/2+             |198.367(10) keV
 32  39 C   |Ge-71m  |20.4 ms                    |9/2+
 32  40 ABC |Ge-72   |STABLE                     |0+
 32  40 AD  |Ge-72m  |444.2(8) ns                |0+               |691.43(4) keV
 32  41 AB  |Ge-73   |STABLE                     |9/2+
 32  41 C   |Ge-73   |>1.8E+23 a                 |9/2+
 32  41 AD  |Ge-73m1 |2.92(3) µs                 |5/2+             |13.2845(15) keV
 32  41 AE  |Ge-73m2 |499(11) ms                 |1/2-             |66.726(9) keV
 32  42 ABC |Ge-74   |STABLE                     |0+
 32  43 ABC |Ge-75   |82.78(4) min               |1/2-
 32  43 AE  |Ge-75m1 |47.7(5) s                  |7/2+             |139.69(3) keV
 32  43 C   |Ge-75m1 |48. s                      |7/2+
 32  43 D   |Ge-75m2 |216(5) ns                  |5/2+             |192.18(7) keV
 32  44 AC  |Ge-76   |1.58(17)E+21 a             |0+
 32  44 B   |Ge-76   |1.2(14)E+25 a              |0+
 32  45 AB  |Ge-77   |11.30(1) h                 |7/2+
 32  45 C   |Ge-77   |11.25 h                    |7/2+
 32  45 AE  |Ge-77m  |52.9(6) s                  |1/2-             |159.70(10) keV
 32  45 C   |Ge-77m  |53. s                      |1/2-
 32  46 AB  |Ge-78   |88(1) min                  |0+
 32  46 C   |Ge-78   |1.45 h                     |0+
 32  47 AB  |Ge-79   |18.98(3) s                 |(1/2)-
 32  47 C   |Ge-79   |19.1 s                     |1/2-
 32  47 AE  |Ge-79m  |39.0(10) s                 |(7/2+)#          |185.95(4) keV
 32  47 C   |Ge-79m  |39. s                      |7/2+
 32  48 ABC |Ge-80   |29.5(4) s                  |0+
 32  49 A   |Ge-81   |8(2)  s                    |9/2+#
 32  49 B   |Ge-81   |7.6(6) s                   |(9/2+)
 32  49 C   |Ge-81   |~7.6 s                     |9/2+
 32  49 A   |Ge-81m  |8(2) s                     |(1/2+)           |679.13(4) keV
 32  49 E   |Ge-81m  |7.6(6) s                   |(1/2+)           |679.13(4) keV
 32  49 C   |Ge-81m  |~7.6 s                     |1/2+
 32  50 ABC |Ge-82   |4.55(5) s                  |0+
 32  51 AB  |Ge-83   |1.85(6) s                  |(5/2+)#
 32  51 C   |Ge-83   |1.9 s                      |
 32  52 A   |Ge-84   |954(14) ms                 |0+
 32  52 B   |Ge-84   |0.947(11) s                |0+
 32  52 C   |Ge-84   |0.98 s                     |
 32  53 A   |Ge-85   |540(50) ms                 |5/2+#
 32  53 B   |Ge-85   |535(47) ms                 |
 32  53 C   |Ge-85   |0.54 s                     |
 32  54 A   |Ge-86   |300# ms [>300 ns]          |0+
 32  54 B   |Ge-86   |>150 ns                    |0+
 32  54 C   |Ge-86   |>0.15 µs                   |
 32  55 A   |Ge-87   |150# ms [>300 ns]          |5/2+#
 32  55 B   |Ge-87   |~0.14 s                    |(5/2+)
 32  55 C   |Ge-87   |>0.15 µs                   |
 32  56 A   |Ge-88   |80# ms [>300 ns]           |0+
 32  56 B   |Ge-88   |>=300 ns                   |0+
 32  56 C   |Ge-88   |>0.15 µs                   |
 32  57 A   |Ge-89   |50# ms [>300 ns]           |3/2+#
 32  57 BC  |Ge-89   |>150 ns                    |

Femto 13:53, 14 November 2005 (UTC)[reply]

Talk

Deleted Reference

I deleted the following:

Because of this, a type of nuclear battery employing germanium and radon (as an alpha source) has been proposed.[1]

  1. ^ "Alpha Fusion Electrical Energy Valve" (PDF). Nu Energy Research Institute. Retrieved 2008-09-10.

As I don't see any evidence that this was anything more than an idea proposed by one group. It also doesn't make much sense as a nuclear battery, since the most stable isotope of radon has a half-life of less than 4 days. It wouldn't last very long, unless you were able to constantly replenish the radon. It seems like you'd want a much longer-lived alpha source. XinaNicole (talk) 06:16, 27 May 2011 (UTC)[reply]

Stability of Germanium EO isotopes

The central mass value stable isotope of 32Ge Germanium is EO32Ge73 with 9 extra neutrons and 7.76% constituency. However as the number of extra neutrons is increased the radioactivity of the OE isotopes is noted to first decrease to 1.38 hours (3.70 log seconds) at EO32Ge75 and then to rise again to 11.25 hours (4.61 log seconds) at EO32Ge77. This is an irregularity in the EO stability data for this element which usually slopes steadily away down the sides of the central tendency of a stability profile chart.WFPM (talk) 01:14, 20 December 2011 (UTC)[reply]

A Log second half-life stability chart of the Wiki data shows clearly this and other stability characteristic tendencies of this (and the other) elements. It is not understood why this method of presenting the reference data is not permitted as a better way to look at and understand this data.17:15, 17 April 2013 (UTC)

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Unclear statement

What does this statement mean?

"Angular momentum or 3rd order sub particles are omitted as spin(2)=0,45,45."

LaundryPizza03 (d) 02:32, 11 May 2018 (UTC)[reply]

"Iso's" button associated with germanium does not function.

I tried the "Iso's" button for many other elements, and they work correctly. 71.8.174.161 (talk) 20:14, 2 October 2019 (UTC)[reply]