镝的同位素
镝(原子量:162.500(1))的同位素中有7個是存在于自然界的穩定同位素,分别是156Dy、158Dy和160Dy至164Dy。自然同位素中豐度最高的是比例為28%的164Dy,緊接著的是比例為26%的162Dy。豐度最低的是比例為0.06%的156Dy。[3]
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
標準原子質量 (Ar, 標準) |
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
通過人工合成,科學家共發現了29種放射性同位素,其原子量在138和173之間。最穩定的是154Dy,其半衰期約為1.40×106年;接著是半衰期為144.4天的159Dy。最不穩定的是138Dy,其半衰期只有200毫秒。比穩定同位素輕的同位素主要進行β+衰變;除個別特例之外,更重的同位素主要進行β−衰變。154Dy主要進行α衰變,152Dy和159Dy則主要進行電子捕獲。[3]鏑擁有至少11種同核異構體(亞穩態),原子量在140和165之間。最穩定的是165mDy,其半衰期為1.257分鐘。149Dy有兩種亞穩態,第二種(149m2Dy)的半衰期只有28納秒。[3]
164Dy是理論上最重的穩定同位素,任何更重的同位素,理論上都會進行α衰變,但是在鉛-208以下,絕大部分的同位素都尚未觀測到此衰變。[4]
圖表
符號 | Z( p ) |
N( n ) |
同位素質量(u) | 半衰期[n 1] | 衰變 方式[5][n 2] |
衰變 產物[n 3] |
原子核 自旋 |
相對豐度 (莫耳分率) |
相對豐度 的變化量 (莫耳分率) |
---|---|---|---|---|---|---|---|---|---|
激發能量 | |||||||||
138Dy | 66 | 72 | 137.96249(64)# | 200# ms | 0+ | ||||
139Dy | 66 | 73 | 138.95954(54)# | 600(200) ms | 7/2+# | ||||
140Dy | 66 | 74 | 139.95401(54)# | 700# ms | β+ | 140Tb | 0+ | ||
140mDy | 2166.1(5) keV | 7.0(5) µs | (8-) | ||||||
141Dy | 66 | 75 | 140.95135(32)# | 0.9(2) s | β+ | 141Tb | (9/2-) | ||
β+, p (不常見) | 140Gd | ||||||||
142Dy | 66 | 76 | 141.94637(39)# | 2.3(3) s | β+ (99.94%) | 142Tb | 0+ | ||
β+, p (.06%) | 141Gd | ||||||||
143Dy | 66 | 77 | 142.94383(21)# | 5.6(10) s | β+ | 143Tb | (1/2+) | ||
β+, p (不常見) | 142Gd | ||||||||
143mDy | 310.7(6) keV | 3.0(3) s | (11/2-) | ||||||
144Dy | 66 | 78 | 143.93925(3) | 9.1(4) s | β+ | 144Tb | 0+ | ||
β+, p (不常見) | 143Gd | ||||||||
145Dy | 66 | 79 | 144.93743(5) | 9.5(10) s | β+ | 145Tb | (1/2+) | ||
β+, p (不常見) | 144Gd | ||||||||
145mDy | 118.2(2) keV | 14.1(7) s | β+ | 145Tb | (11/2-) | ||||
146Dy | 66 | 80 | 145.932845(29) | 33.2(7) s | β+ | 146Tb | 0+ | ||
146mDy | 2935.7(6) keV | 150(20) ms | IT | 146Dy | (10+)# | ||||
147Dy | 66 | 81 | 146.931092(21) | 40(10) s | β+ (99.95%) | 147Tb | 1/2+ | ||
β+, p (.05%) | 146Tb | ||||||||
147m1Dy | 750.5(4) keV | 55(1) s | β+ (65%) | 147Tb | 11/2- | ||||
IT (35%) | 147Dy | ||||||||
147m2Dy | 3407.2(8) keV | 0.40(1) µs | (27/2-) | ||||||
148Dy | 66 | 82 | 147.927150(11) | 3.3(2) min | β+ | 148Tb | 0+ | ||
149Dy | 66 | 83 | 148.927305(9) | 4.20(14) min | β+ | 149Tb | 7/2(-) | ||
149mDy | 2661.1(4) keV | 490(15) ms | IT (99.3%) | 149Dy | (27/2-) | ||||
β+ (.7%) | 149Tb | ||||||||
150Dy | 66 | 84 | 149.925585(5) | 7.17(5) min | β+ (64%) | 150Tb | 0+ | ||
α (36%) | 146Gd | ||||||||
151Dy | 66 | 85 | 150.926185(4) | 17.9(3) min | β+ (94.4%) | 151Tb | 7/2(-) | ||
α (5.6%) | 147Gd | ||||||||
152Dy | 66 | 86 | 151.924718(6) | 2.38(2) h | ε (99.9%) | 152Tb | 0+ | ||
α (.1%) | 148Gd | ||||||||
153Dy | 66 | 87 | 152.925765(5) | 6.4(1) h | β+ (99.99%) | 153Tb | 7/2(-) | ||
α (.00939%) | 149Gd | ||||||||
154Dy | 66 | 88 | 153.924424(8) | 3.0(15)×106 a | α | 150Gd | 0+ | ||
155Dy | 66 | 89 | 154.925754(13) | 9.9(2) h | β+ | 155Tb | 3/2- | ||
155mDy | 234.33(3) keV | 6(1) µs | 11/2- | ||||||
156Dy | 66 | 90 | 155.924283(7) | 觀測上穩定[n 4] | 0+ | 5.6(3)×10−4 | |||
157Dy | 66 | 91 | 156.925466(7) | 8.14(4) h | β+ | 157Tb | 3/2- | ||
157m1Dy | 161.99(3) keV | 1.3(2) µs | 9/2+ | ||||||
157m2Dy | 199.38(7) keV | 21.6(16) ms | IT | 157Dy | 11/2- | ||||
158Dy | 66 | 92 | 157.924409(4) | 觀測上穩定[n 5] | 0+ | 9.5(3)×10−4 | |||
159Dy | 66 | 93 | 158.9257392(29) | 144.4(2) d | ε | 159Tb | 3/2- | ||
159mDy | 352.77(14) keV | 122(3) µs | 11/2- | ||||||
160Dy | 66 | 94 | 159.9251975(27) | 觀測上穩定[n 6] | 0+ | 0.02329(18) | |||
161Dy | 66 | 95 | 160.9269334(27) | 觀測上穩定[n 7] | 5/2+ | 0.18889(42) | |||
162Dy | 66 | 96 | 161.9267984(27) | 觀測上穩定[n 8] | 0+ | 0.25475(36) | |||
163Dy | 66 | 97 | 162.9287312(27) | 稳定[n 9][6] | 5/2- | 0.24896(42) | |||
164Dy | 66 | 98 | 163.9291748(27) | 稳定 | 0+ | 0.28260(54) | |||
165Dy | 66 | 99 | 164.9317033(27) | 2.334(1) h | β− | 165Ho | 7/2+ | ||
165mDy | 108.160(3) keV | 1.257(6) min | IT (97.76%) | 165Dy | 1/2- | ||||
β− (2.24%) | 165Ho | ||||||||
166Dy | 66 | 100 | 165.9328067(28) | 81.6(1) h | β− | 166Ho | 0+ | ||
167Dy | 66 | 101 | 166.93566(6) | 6.20(8) min | β− | 167Ho | (1/2-) | ||
168Dy | 66 | 102 | 167.93713(15) | 8.7(3) min | β− | 168Ho | 0+ | ||
169Dy | 66 | 103 | 168.94031(32) | 39(8) s | β− | 169Ho | (5/2-) | ||
170Dy | 66 | 104 | 169.94239(21)# | 30# s | β− | 170Ho | 0+ | ||
171Dy | 66 | 105 | 170.94620(32)# | 6# s | β− | 171Ho | 7/2-# | ||
172Dy | 66 | 106 | 171.94876(43)# | 3# s | β− | 172Ho | 0+ | ||
173Dy | 66 | 107 | 172.95300(54)# | 2# s | β− | 173Ho | 9/2+# |
備註:畫上#號的數據代表沒有經過實驗的証明,只是理論推測而已,而用括號括起來的代表數據不確定性。
← | 同位素列表 | → |
鋱的同位素 | 镝的同位素 | 鈥的同位素 |
註釋
- Bold for isotopes with half-lives longer than the age of the universe (nearly stable)
- Abbreviations:
ε: Electron capture
IT: Isomeric transition - Bold for stable isotopes, bold italics for nearly stable isotopes (half-life longer than the age of the universe)
- Believed to undergo α decay to 152Gd or β+β+ decay to 156Gd with a half-life over 1018 years
- Believed to undergo α decay to 154Gd or β+β+ decay to 158Gd
- Believed to undergo α decay to 156Gd
- Believed to undergo α decay to 157Gd
- Believed to undergo α decay to 158Gd
- Can undergo [[Beta_decay#Bound-state_β−_decay|bound-state β− decay]] to 163Ho with a half-life of 47 days when fully ionized
参考文獻
- Chiera, Nadine Mariel; Dressler, Rugard; Sprung, Peter; Talip, Zeynep; Schumann, Dorothea. . Scientific Reports (Springer Science and Business Media LLC). 2022-05-28, 12 (1). ISSN 2045-2322. doi:10.1038/s41598-022-12684-6.
- Meija, Juris; et al. . Pure and Applied Chemistry. 2016, 88 (3): 265–91. doi:10.1515/pac-2015-0305.
- Audi, G.; Bersillon, O.; Blachot, J.; Wapstra, A.H. . Nuclear Physics A (Atomic Mass Data Center). 2003, 729: 3–128. Bibcode:2003NuPhA.729....3A. doi:10.1016/j.nuclphysa.2003.11.001.
- Belli, P.; Bernabei, R.; Danevich, F.A.; Incicchitti, A.; Tretyak, V.I. . Eur. Phys. J. A. August 2019, 55: 140. doi:10.1140/epja/i2019-12823-2.
- . [2015-09-20]. (原始内容存档于2017-02-19).
- M. Jung et al., Phys. Rev. Letts. 69, 2164 (1992) First observation of bound-state beta minus decay.
- Isotope masses from Ame2003 Atomic Mass Evaluation by G. Audi, A.H. Wapstra, C. Thibault, J. Blachot and O. Bersillon in Nuclear Physics A729 (2003).
- Isotopic compositions and standard atomic masses from Atomic weights of the elements. Review 2000 (IUPAC Technical Report) (页面存档备份,存于). Pure Appl. Chem. Vol. 75, No. 6, pp. 683-800, (2003) and Atomic Weights Revised (2005) (页面存档备份,存于).
- Half-life, spin, and isomer data selected from these sources. Editing notes on this article's talk page.
- Audi, Bersillon, Blachot, Wapstra. The Nubase2003 evaluation of nuclear and decay properties (页面存档备份,存于), Nuc. Phys. A 729, pp. 3-128 (2003).
- National Nuclear Data Center, Brookhaven National Laboratory. Information extracted from the NuDat 2.1 database (页面存档备份,存于) (retrieved Sept. 2005).
- 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.
This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.