51
Sb
Antimony
Atomic Mass 121.760
Electron Configuration [Kr]5s24d105p3
Oxidation States +5, +3, -3
Year Discovered Ancient

Identifiers

Element Name Antimony
Element Symbol Sb
InChI InChI=1S/Sb
InChIKey WATWJIUSRGPENY-UHFFFAOYSA-N

Properties

Atomic Weight

121.760(1)

121.760

121.8

121.760(1)

Electron Configuration

[Kr]5s24d105p3

Atomic Radius

Van der Waals Atomic Radius : 206 pm (Van der Waals)

Empirical Atomic Radius : 145pm (Empirical)

Covalent Atomic Radius : 139(5) pm (Covalent)

Oxidation States

+5, +3, -3

5, 4, 3, 2, 1, -1, -2, -3 ​(an amphoteric oxide)

Ground Level

43/2

Ionization Energy

8.64 eV

8.608389 ± 0.000012 eV

Electronegativity

Pauling Scale Electronegativity : 2.05(Pauling Scale)

Allen Scale Electronegativity : 1.984(Allen Scale)

Electron Affinity

1.07eV

0.94eV

Atomic Spectra

Lines Holdings

Levels Holdings

Physical Description

Solid

Element Classification

Semi-metal

Element Period Number

5

Element Group Number

15 - Pnictogen

Density

6.685 grams per cubic centimeter

Melting Point

903.78 K (630.63°C or 1167.13°F)

630.63°C

Boiling Point

1860 K (1587°C or 2889°F)

1635°C

Estimated Crustal Abundance

2×10-1 milligrams per kilogram

Estimated Oceanic Abundance

2.4×10-4 milligrams per liter

History

The name derives from the Greek, anti + monos for "not alone" or "not one" because it was found in many compounds. The symbol Sb comes from stibium, which is derived from the Greek stibi for "mark" because it was used for blackening eyebrows and eyelashes. The minerals stibnite (Sb2S3) and stibine (SbH3) are two of more than one hundred mineral species, which were known in the ancient world.

Antimony has been known since ancient times. It is sometimes found free in nature, but is usually obtained from the ores stibnite (Sb2S3) and valentinite (Sb2O3). Nicolas Lémery, a French chemist, was the first person to scientifically study antimony and its compounds. He published his findings in 1707. Antimony makes up about 0.00002% of the earth's crust.

From the Greek word anti plus monos - "a metal not found alone". Antimony was recognized in compounds by the ancients and was known as a metal at the beginning of the 17th century and possibly much earlier.

Historical Atomic Weights

Year Atomic Weight (uncertainty) [u] Reference
1993 121.760(1) https://doi.org/10.1351/pac199466122423
1989 121.757(3) https://doi.org/10.1351/pac199163070975
1969 121.75(3) https://doi.org/10.1351/pac197021010091
1961 121.75 https://doi.org/10.1021/ja00881a001
1931 121.76 https://doi.org/10.1039/JR9310001617
1925 121.77 https://doi.org/10.1039/CT9252700913
1903 120.2 https://doi.org/10.1021/ja02003a001
1902 120.0 https://doi.org/10.1007/BF01370337

Historical Isotopic Abundances

Year Isotope Abundance (uncertainty) Reference
1997 121Sb 0.5721(5) https://doi.org/10.1351/pac199870010217
1997 123Sb 0.4279(5) https://doi.org/10.1351/pac199870010217
1989 121Sb 0.5736(8) https://doi.org/10.1351/pac199163070991
1989 123Sb 0.4264(8) https://doi.org/10.1351/pac199163070991
1979 121Sb 0.573(9) https://doi.org/10.1351/pac198052102349
1979 123Sb 0.427(9) https://doi.org/10.1351/pac198052102349
1975 121Sb 0.573 https://doi.org/10.1351/pac197647010075
1975 123Sb 0.427 https://doi.org/10.1351/pac197647010075

Description

Antimony is a poor conductor of heat and electricity. Antimony and many of its compounds are toxic.

Users

Antimony is a brittle metal and is a poor conductor of heat and electricity. Very pure antimony is used to make certain types of semiconductor devices, such as diodes and infrared detectors. Antimony is alloyed with lead to increase lead's durability. Antimony alloys are also used in batteries, low friction metals, type metal and cable sheathing, among other products. Antimony compounds are used to make flame-proofing materials, paints, ceramic enamels, glass and pottery. The ancient Egyptians used antimony, in the form of stibnite, for black eye make-up.

Antimony is finding use in semiconductor technology for making infrared detectors, diodes and Hall-effect devices. It greatly increases the hardness and mechanical strength of lead. Batteries, antifriction alloys, type metal, small arms and tracer bullets, cable sheathing, and minor products use about half the metal produced. Compounds taking up the other half are oxides, sulfides, sodium antimonate, and antimony trichloride. These are used in manufacturing flame-proofing compounds, paints ceramic enamels, glass, and pottery.

Sources

Antimony is not abundant, but is found in over 100 mineral species. It is sometimes found natively, but more frequently it is found as the sulfide stibnite.

Compounds

See more information at the Antimony compound page.

Element Forms

CID Name Formula SMILES Molecular Weight
5354495 antimony Sb [Sb] 121.760
104894 antimony(3+) Sb+3 [Sb+3] 121.760
73608879 antimony(5+) Sb+5 [Sb+5] 121.760
6335317 antimony-125 Sb [125Sb] 124.90525
6335510 antimony-124 Sb [124Sb] 123.90594
6337074 antimony-117 Sb [117Sb] 116.90484
6337563 antimony-119 Sb [119Sb] 118.90394
25087156 antimony-121 Sb [121Sb] 120.90381
6335314 antimony-127 Sb [127Sb] 126.90693
6335836 antimony-122 Sb [122Sb] 121.90517
6337042 antimony-129 Sb [129Sb] 128.9091
6337048 antimony-120 Sb [120Sb] 119.90508
6337079 antimony-131 Sb [131Sb] 130.91199
6337080 antimony-126 Sb [126Sb] 125.9073
6337082 antimony-130 Sb [130Sb] 129.9117
42626464 antimony-123 Sb [123Sb] 122.90422
6337075 antimony-116 Sb [116Sb] 115.90679
6337081 antimony-128 Sb [128Sb] 127.9091
6337534 antimony-115 Sb [115Sb] 114.9066
6337545 antimony-118 Sb [118Sb] 117.90553
51352723 antimony-126(3+) Sb+3 [126Sb+3] 125.9073
51352724 antimony-127(3+) Sb+3 [127Sb+3] 126.90693

Isotopes

Stable Isotope Count 2

Isotopes in Earth/Planetary Science

Molecules, atoms, and ions of the stable isotopes of antimony possess slightly different physical and chemical properties, and they commonly will be fractionated during physical, chemical, and biological processes, giving rise to variations in isotopic abundances and in atomic weights. There are measureable substantial variations in the isotopic abundances of antimony in natural terrestrial materials (Fig. IUPAC.51.1) [370]. The stable isotopes 121Sb and 123Sb have been used to measure movement of sediments and rocks originating from locations high in antimony. 121Sb and 123Sb move with the sediments and have been used as tracers in areas low in antimony to determine the originating location of certain metal/metalloid contaminants in streams [371], [372], [373].

Fig. IUPAC.51.1: Variation in isotope-amount ratio n(¹²³Sb)/n(¹²¹Sb) of antimony in terrestrial materials (modified from [370]), assuming a measured isotope-amount ratio n(¹²³Sb)/n(¹²¹Sb) of 0.747 85 [374].

[370] O. Rouxel, J. Ludden, Y. Fouquet. Chem. Geol.200, 25 (2003).
[371] B. Chauvenet, M. M. Be, M. N. Amiot, C. Bobin, M. C. Lepy, T. Branger, I. Laniece, A. Luca, M. Sahagia, A. C. Watjen, K. Kossert, O. Ott, O. Nahle, P. Dryak, J. Sochorova, P. Kovar, P. Auerbach, T. Altzitzoglou, S. Pomme, G. Sibbens, R. Van Ammel, J. Paepen, A. Iwahara, J. U. Delgado, R. Poledna, C. J. da Silva, L. Johansson, A. Stroak, C. Bailat, Y. Nedjadi, P. Spring. Appl. Radiat. Isot.68, 1207 (2010).
[372] M. Baeza, J. Ren, S. Krishnamurthy, T. C. Vaughan. Arch. Environ. Contam. Toxicol.8, 299 (2010).
[373] L. Wilson. “Determination of trace element provenance in the Rio Loa Basin, Chile”, in 2010 Geological Society of America Presentation.
[374] T. L. Chang, Q. Y. Qian, M. T. Zhao, J. Wang. Int. J. Mass Spectrom. Ion Processes123, 77 (1993).

Isotopes in Industry

In the 1950s, 124Sb and 125Sb (with half-lives of 60 days and about 1000 days, respectively) were used commercially as tracers. They were injected into oil pipelines as a way to detect the residence time and flow rate of the substance through the pipeline. The presence of these isotopes could be detected by means of a Geiger counter held above the pipeline. If the pipeline had a leak, the tracer would escape and its contamination and movement could be detected in the soil. 124Sb and 125Sb are now both treated as environmental contaminants [375].

[375] R. Gibbs. Popular Mech.117, 117 (1955).

Isotopes Used as a Source of Radioactive Isotope(s)

123Sb is used to produce 124I (with a half-life of 100 h), which is used in radioimmunotherapy and also in positron emission tomography. It can be produced from the 123Sb (3He, 2n) 124I reaction [376]. 121Sb and 123Sb can both be used for the production of 123I (with a half-life of 13.2 h) via 3He and alpha particle-induced reactions with 121Sb and 123Sb, although the most common production route is via 124Xe or 123Te [377].

[376] M. S. Uddin, A. Hermanne, S. Sudár, M. N. Aslam, B. Scholten, H. H. Coenen, S. M. Qaim. Appl. Radiat. Isot.69, 699 (2010).
[377] K. F. Hassan, S. M. Qaim, Z. A. Saleh, H. H. Coenen. Appl. Radiat. Isot.64, 101 (2006).

Isotope Mass and Abundance

Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
121Sb 120.903 81(2) 0.5721(5)
123Sb 122.904 21(1) 0.4279(5)
Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
121Sb 120.9038120(30) 0.5721(5)
123Sb 122.9042132(23) 0.4279(5)

Atomic Mass, Half Life, and Decay

Nuclide Atomic Mass and Uncertainty [u] Half Life and Uncertainty Discovery Year Decay Modes, Intensities and Uncertainties [%]
102Sb 101.945142 ± 0.000429 [Estimated] Not-specified p ?
103Sb 102.939162 ± 0.000322 [Estimated] Not-specified <49ns 2010 p ?
104Sb 103.936344 ± 0.000109 [Estimated] 470 ms ± 130 1995 β+=?; β+p<7%; p<7%; α ?
105Sb 104.931276547 ± 0.000023431 1.12 s ± 0.16 1994 β+=100%; p<0.1%; β+p ?
106Sb 105.928637979 ± 0.000008 600 ms ± 200 1981 β+=100%
106Sbm 105.928637979 ± 0.000008 226 ns ± 14 1998 IT=100%
107Sb 106.924150621 ± 0.000004452 4.0 s ± 0.2 1994 β+=100%
108Sb 107.922226731 ± 0.0000059 7.4 s ± 0.3 1976 β+=100%
109Sb 108.918141203 ± 0.000005652 17.2 s ± 0.5 1976 β+=100%
110Sb 109.916854283 ± 0.0000064 23.6 s ± 0.3 1972 β+=100%
111Sb 110.913218187 ± 0.0000095 75 s ± 1 1972 β+=100%
112Sb 111.912399903 ± 0.00001914 53.5 s ± 0.6 1959 β+=100%
112Sbm 111.912399903 ± 0.00001914 536 ns ± 22 1976 IT=100%
113Sb 112.909374664 ± 0.000018457 6.67 m ± 0.07 1958 β+=100%
114Sb 113.909289155 ± 0.000021226 3.49 m ± 0.03 1959 β+=100%
114Sbm 113.909289155 ± 0.000021226 219 us ± 12 1973 IT=100%
115Sb 114.906598000 ± 0.000017203 32.1 m ± 0.3 1958 β+=100%
115Sbm 114.906598000 ± 0.000017203 159 ns ± 3 1977 IT=100%
116Sb 115.906792732 ± 0.000005533 15.8 m ± 0.8 1949 β+=100%
116Sbm 115.906792732 ± 0.000005533 194 ns ± 4 1976 IT=100%
116Sbn 115.906792732 ± 0.000005533 60.3 m ± 0.6 1949 β+=100%
117Sb 116.904841519 ± 0.000009057 2.97 h ± 0.02 1947 β+=100%
117Sbm 116.904841519 ± 0.000009057 355 us ± 17 1970 IT=100%
117Sbn 116.904841519 ± 0.000009057 290 ns ± 5 1987 IT=100%
118Sb 117.905532194 ± 0.000003237 3.6 m ± 0.1 1947 β+=100%
118Sbm 117.905532194 ± 0.000003237 20.6 us ± 0.6 1975 IT=100%
118Sbn 117.905532194 ± 0.000003237 5.01 h ± 0.03 1947 β+=100%
119Sb 118.903944062 ± 0.000007512 38.19 h ± 0.22 1947 ε=100%
119Sbm 118.903944062 ± 0.000007512 130 ns ± 3 1991 IT=100%
119Sbn 118.903944062 ± 0.000007512 835 ms ± 81 1979 IT=100%
120Sb 119.905080308 ± 0.000007728 15.89 m ± 0.04 1937 β+=100%
120Sbm 119.905080308 ± 0.000007728 5.76 d ± 0.02 1958 β+=100%
120Sbn 119.905080308 ± 0.000007728 246 ns ± 2 1976 IT=100%
120Sbp 119.905080308 ± 0.000007728 400 ns ± 8 1983 IT=100%
121Sb 120.903811353 ± 0.00000269 Stable 1922 IS=57.21±0.5%
121Sbm 120.903811353 ± 0.00000269 179 us ± 6 2008 IT=100%
122Sb 121.905169335 ± 0.000002687 2.7238 d ± 0.0002 1939 β-=97.59±1.2%; β+=2.41±1.2%
122Sbm 121.905169335 ± 0.000002687 1.86 us ± 0.08 1962 IT=100%
122Sbn 121.905169335 ± 0.000002687 530 us ± 30 1963 IT=100%
122Sbp 121.905169335 ± 0.000002687 4.191 m ± 0.003 1947 IT=100%
123Sb 122.904215292 ± 0.000001456 Stable 1922 IS=42.79±0.5%
123Sbm 122.904215292 ± 0.000001456 214 ns ± 3 2005 IT=100%
123Sbn 122.904215292 ± 0.000001456 65 us ± 1 2007 IT=100%
124Sb 123.905937065 ± 0.000001457 60.20 d ± 0.03 1939 β-=100%
124Sbm 123.905937065 ± 0.000001457 93 s ± 5 1947 IT=75±0.5%; β-=25±0.5%
124Sbn 123.905937065 ± 0.000001457 20.2 m ± 0.2 1947 IT=100[gs=0,m=100]
124Sbp 123.905937065 ± 0.000001457 3.2 us ± 0.3 1989 IT=100%
125Sb 124.905254264 ± 0.0000027 2.7576 y ± 0.0011 1951 β-=100%
125Sbm 124.905254264 ± 0.0000027 4.1 us ± 0.2 2007 IT=100%
125Sbn 124.905254264 ± 0.0000027 28.5 us ± 0.5 2007 IT=100%
125Sbq 124.905254264 ± 0.0000027 277.0 ns ± 6.4 2007 IT=100%
126Sb 125.907253158 ± 0.000034189 12.35 d ± 0.06 1956 β-=100%
126Sbm 125.907253158 ± 0.000034189 19.15 m ± 0.08 1956 β-=86±0.4%; IT=14±0.4%
126Sbn 125.907253158 ± 0.000034189 ~11 s 1976 IT=100[gs=0,m=100]
126Sbp 125.907253158 ± 0.000034189 553 ns ± 5 1976 IT=100%
126Sbq 125.907253158 ± 0.000034189 90 ns ± 16 2019 IT=100%
127Sb 126.906925557 ± 0.000005457 3.85 d ± 0.05 1939 β-=100%
127Sbm 126.906925557 ± 0.000005457 11.7 us ± 0.1 1974 IT=100%
127Sbn 126.906925557 ± 0.000005457 269 ns ± 5 2005 IT=100%
128Sb 127.909146121 ± 0.000020169 9.05 h ± 0.04 1956 β-=100%
128Sbm 127.909146121 ± 0.000020169 10.41 m ± 0.18 1955 β-=96.4±1%; IT=3.6±1%
128Sbn 127.909146121 ± 0.000020169 500 ns ± 20 2019 IT=100%
128Sbp 127.909146121 ± 0.000020169 217 ns ± 7 2019 IT=100%
129Sb 128.909146623 ± 0.000022786 4.366 h ± 0.026 1939 β-=100%
129Sbm 128.909146623 ± 0.000022786 17.7 m ± 0.1 1982 β-=85%; IT=15%
129Sbn 128.909146623 ± 0.000022786 2.23 us ± 0.17 1987 IT=100%
129Sbp 128.909146623 ± 0.000022786 0.89 us ± 0.03 2003 IT=100%
130Sb 129.911662686 ± 0.000015257 39.5 m ± 0.8 1962 β-=100%
130Sbm 129.911662686 ± 0.000015257 6.3 m ± 0.2 1962 β-=100%
130Sbn 129.911662686 ± 0.000015257 800 ns ± 100 2002 IT=100%
130Sbp 129.911662686 ± 0.000015257 600 ns ± 15 2019 IT=100%
130Sbq 129.911662686 ± 0.000015257 1.25 us ± 0.01 2002 IT=100%
131Sb 130.911989339 ± 0.000002236 23.03 m ± 0.04 1956 β-=100%
131Sbm 130.911989339 ± 0.000002236 64.2 us ± 2.6 1969 IT=100%
131Sbn 130.911989339 ± 0.000002236 4.3 us ± 0.8 2000 IT=100%
131Sbp 130.911989339 ± 0.000002236 0.97 us ± 0.03 2000 IT=100%
132Sb 131.914508013 ± 0.000002648 2.79 m ± 0.07 1956 β-=100%
132Sbm 131.914508013 ± 0.000002648 4.10 m ± 0.05 1956 β-=100%
132Sbn 131.914508013 ± 0.000002648 102 ns ± 4 1974 IT=100%
133Sb 132.915272128 ± 0.000003357 2.34 m ± 0.05 1966 β-=100%
133Sbm 132.915272128 ± 0.000003357 16.54 us ± 0.19 1978 IT=100%
134Sb 133.920537334 ± 0.0000033 674 ms ± 4 1967 β-=100%; β-n ?
134Sbm 133.920537334 ± 0.0000033 10.01 s ± 0.04 1968 β-=100%; β-n=0.088±0.4%
135Sb 134.925184354 ± 0.000002834 1.668 s ± 0.009 1964 β-=100%; β-n=19.1±0.5%
136Sb 135.930749009 ± 0.000006258 923 ms ± 14 1976 β-=100%; β-n=24.7±0.5%; β-2n=0.14±0.3%
136Sbm 135.930749009 ± 0.000006258 570 ns ± 5 2001 IT=100%
137Sb 136.935522519 ± 0.000056 497 ms ± 21 1994 β-=100%; β-n=49±0.6%; β-2n ?
138Sb 137.941331 ± 0.000322 [Estimated] 333 ms ± 7 1994 β-=100%; β-n=72±0.8%; β-2n ?
139Sb 138.946269 ± 0.000429 [Estimated] 182 ms ± 9 1994 β-=100%; β-n=90±1%; β-2n ?
140Sb 139.952345 ± 0.000644 [Estimated] 170 ms ± 6 2010 β-=100%; β-n=23±0.4%; β-2n=7.6±2.5%
140Sbm 139.952345 ± 0.000644 [Estimated] 41 us ± 8 2016 IT=100%
141Sb 140.957552 ± 0.000537 [Estimated] 103 ms ± 29 2018 β-=100%; β-n ?; β-2n ?
142Sb 141.963918 ± 0.000322 [Estimated] 80 ms ± 50 2018 β-=100%; β-n ?; β-2n ?

Information Sources

  1. 1.  PubChem
  2. 2.  Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
  3. 3.  IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)
  4. 4.  Jefferson Lab, U.S. Department of Energy
    LICENSE
    Please see citation and linking information https https://www.jlab.org/privacy-and-security-notice
  5. 5.  Los Alamos National Laboratory, U.S. Department of Energy
  6. 6.  NIST Physical Measurement Laboratory
  7. 7.  IUPAC Periodic Table of the Elements and Isotopes (IPTEI)
    LICENSE
    Copyright (c) 2020 International Union of Pure and Applied Chemistry. The International Union of Pure and Applied Chemistry (IUPAC) contribution within Pubchem is provided under a CC-BY-NC-ND 4.0 license, unless otherwise stated.
    https://creativecommons.org/licenses/by-nc-nd/4.0/
  8. 8.  PubChem Elements
    Antimony

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