Palladium 103
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Naturally occurring
palladium Palladium is a chemical element with the symbol Pd and atomic number 46. It is a rare and lustrous silvery-white metal discovered in 1803 by the English chemist William Hyde Wollaston. He named it after the asteroid Pallas, which was itself na ...
(46Pd) is composed of six stable
isotope Isotopes are two or more types of atoms that have the same atomic number (number of protons in their nuclei) and position in the periodic table (and hence belong to the same chemical element), and that differ in nucleon numbers (mass numb ...
s, 102Pd, 104Pd, 105Pd, 106Pd, 108Pd, and 110Pd, although 102Pd and 110Pd are theoretically unstable. The most stable
radioisotope A radionuclide (radioactive nuclide, radioisotope or radioactive isotope) is a nuclide that has excess nuclear energy, making it unstable. This excess energy can be used in one of three ways: emitted from the nucleus as gamma radiation; transferr ...
s are 107Pd with a
half-life Half-life (symbol ) is the time required for a quantity (of substance) to reduce to half of its initial value. The term is commonly used in nuclear physics to describe how quickly unstable atoms undergo radioactive decay or how long stable at ...
of 6.5 million years, 103Pd with a half-life of 17 days, and 100Pd with a half-life of 3.63 days. Twenty-three other radioisotopes have been characterized with
atomic weight Relative atomic mass (symbol: ''A''; sometimes abbreviated RAM or r.a.m.), also known by the deprecated synonym atomic weight, is a dimensionless physical quantity defined as the ratio of the average mass of atoms of a chemical element in a giv ...
s ranging from 90.949 u (91Pd) to 128.96 u (129Pd). Most of these have half-lives that are less than a half an hour except 101Pd (half-life: 8.47 hours), 109Pd (half-life: 13.7 hours), and 112Pd (half-life: 21 hours). The primary decay mode before the most abundant stable isotope, 106Pd, is
electron capture Electron capture (K-electron capture, also K-capture, or L-electron capture, L-capture) is a process in which the proton-rich nucleus of an electrically neutral atom absorbs an inner atomic electron, usually from the K or L electron shells. Thi ...
and the primary mode after is
beta decay In nuclear physics, beta decay (β-decay) is a type of radioactive decay in which a beta particle (fast energetic electron or positron) is emitted from an atomic nucleus, transforming the original nuclide to an isobar of that nuclide. For ...
. The primary decay product before 106Pd is
rhodium Rhodium is a chemical element with the symbol Rh and atomic number 45. It is a very rare, silvery-white, hard, corrosion-resistant transition metal. It is a noble metal and a member of the platinum group. It has only one naturally occurring i ...
and the primary product after is
silver Silver is a chemical element with the symbol Ag (from the Latin ', derived from the Proto-Indo-European ''h₂erǵ'': "shiny" or "white") and atomic number 47. A soft, white, lustrous transition metal, it exhibits the highest electrical ...
.
Radiogenic A radiogenic nuclide is a nuclide that is produced by a process of radioactive decay. It may itself be radioactive (a radionuclide) or stable (a stable nuclide). Radiogenic nuclides (more commonly referred to as radiogenic isotopes) form some ...
107Ag is a decay product of 107Pd and was first discovered in the Santa Clara meteorite of 1978. The discoverers suggest that the coalescence and differentiation of iron-cored small planets may have occurred 10 million years after a
nucleosynthetic Nucleosynthesis is the process that creates new atomic nuclei from pre-existing nucleons (protons and neutrons) and nuclei. According to current theories, the first nuclei were formed a few minutes after the Big Bang, through nuclear reactions in ...
event. 107Pd versus Ag correlations observed in bodies, which have clearly been melted since accretion of the
Solar System The Solar System Capitalization of the name varies. The International Astronomical Union, the authoritative body regarding astronomical nomenclature, specifies capitalizing the names of all individual astronomical objects but uses mixed "Solar ...
, must reflect the presence of short-lived nuclides in the early Solar System.


List of isotopes

, - , 91Pd , style="text-align:right" , 46 , style="text-align:right" , 45 , 90.94911(61)# , 10# ms 1.5 µs, β+ , 91Rh , 7/2+# , , , - , 92Pd , style="text-align:right" , 46 , style="text-align:right" , 46 , 91.94042(54)# , 1.1(3) s .7(+4−2) s, β+ , 92Rh , 0+ , , , - , 93Pd , style="text-align:right" , 46 , style="text-align:right" , 47 , 92.93591(43)# , 1.07(12) s , β+ , 93Rh , (9/2+) , , , - , style="text-indent:1em" , 93mPd , colspan="3" style="text-indent:2em" , 0+X keV , 9.3(+25−17) s , , , , , , - , 94Pd , style="text-align:right" , 46 , style="text-align:right" , 48 , 93.92877(43)# , 9.0(5) s , β+ , 94Rh , 0+ , , , - , style="text-indent:1em" , 94mPd , colspan="3" style="text-indent:2em" , 4884.4(5) keV , 530(10) ns , , , (14+) , , , - , 95Pd , style="text-align:right" , 46 , style="text-align:right" , 49 , 94.92469(43)# , 10# s , β+ , 95Rh , 9/2+# , , , - , rowspan=3 style="text-indent:1em" , 95mPd , rowspan=3 colspan="3" style="text-indent:2em" , 1860(500)# keV , rowspan=3, 13.3(3) s , β+ (94.1%) , 95Rh , rowspan=3, (21/2+) , rowspan=3, , rowspan=3, , - , IT (5%) , 95Pd , - , β+, p (.9%) , 94Ru , - , 96Pd , style="text-align:right" , 46 , style="text-align:right" , 50 , 95.91816(16) , 122(2) s , β+ , 96Rh , 0+ , , , - , style="text-indent:1em" , 96mPd , colspan="3" style="text-indent:2em" , 2530.8(1) keV , 1.81(1) µs , , , 8+ , , , - , 97Pd , style="text-align:right" , 46 , style="text-align:right" , 51 , 96.91648(32) , 3.10(9) min , β+ , 97Rh , 5/2+# , , , - , 98Pd , style="text-align:right" , 46 , style="text-align:right" , 52 , 97.912721(23) , 17.7(3) min , β+ , 98Rh , 0+ , , , - , 99Pd , style="text-align:right" , 46 , style="text-align:right" , 53 , 98.911768(16) , 21.4(2) min , β+ , 99Rh , (5/2)+ , , , - , 100Pd , style="text-align:right" , 46 , style="text-align:right" , 54 , 99.908506(12) , 3.63(9) d , EC , 100Rh , 0+ , , , - , 101Pd , style="text-align:right" , 46 , style="text-align:right" , 55 , 100.908289(19) , 8.47(6) h , β+ , 101Rh , 5/2+ , , , - , 102Pd , style="text-align:right" , 46 , style="text-align:right" , 56 , 101.905609(3) , colspan=3 align=center,
Observationally Stable Stable nuclides are nuclides that are not radioactive and so (unlike radionuclides) do not spontaneously undergo radioactive decay. When such nuclides are referred to in relation to specific elements, they are usually termed stable isotopes. Th ...
Believed to decay by β+β+ to 102Ru , 0+ , 0.0102(1) , , - , 103PdUsed in medicine , style="text-align:right" , 46 , style="text-align:right" , 57 , 102.906087(3) , 16.991(19) d , EC , 103Rh , 5/2+ , , , - , style="text-indent:1em" , 103mPd , colspan="3" style="text-indent:2em" , 784.79(10) keV , 25(2) ns , , , 11/2− , , , - , 104Pd , style="text-align:right" , 46 , style="text-align:right" , 58 , 103.904036(4) , colspan=3 align=center, StableTheoretically capable of spontaneous fission , 0+ , 0.1114(8) , , - , 105Pd Fission product , style="text-align:right" , 46 , style="text-align:right" , 59 , 104.905085(4) , colspan=3 align=center, Stable , 5/2+ , 0.2233(8) , , - , 106Pd , style="text-align:right" , 46 , style="text-align:right" , 60 , 105.903486(4) , colspan=3 align=center, Stable , 0+ , 0.2733(3) , , - , 107Pd Long-lived fission product , style="text-align:right" , 46 , style="text-align:right" , 61 , 106.905133(4) , 6.5(3)×106 y , β , 107Ag , 5/2+ , trace
Cosmogenic Cosmogenic nuclides (or cosmogenic isotopes) are rare nuclides (isotopes) created when a high-energy cosmic ray interacts with the nucleus of an ''in situ'' Solar System atom, causing nucleons (protons and neutrons) to be expelled from the atom ...
nuclide, also found as nuclear contamination
, , - , style="text-indent:1em" , 107m1Pd , colspan="3" style="text-indent:2em" , 115.74(12) keV , 0.85(10) µs , , , 1/2+ , , , - , style="text-indent:1em" , 107m2Pd , colspan="3" style="text-indent:2em" , 214.6(3) keV , 21.3(5) s , IT , 107Pd , 11/2− , , , - , 108Pd , style="text-align:right" , 46 , style="text-align:right" , 62 , 107.903892(4) , colspan=3 align=center, Stable , 0+ , 0.2646(9) , , - , 109Pd , style="text-align:right" , 46 , style="text-align:right" , 63 , 108.905950(4) , 13.7012(24) h , β , 109mAg , 5/2+ , , , - , style="text-indent:1em" , 109m1Pd , colspan="3" style="text-indent:2em" , 113.400(10) keV , 380(50) ns , , , 1/2+ , , , - , style="text-indent:1em" , 109m2Pd , colspan="3" style="text-indent:2em" , 188.990(10) keV , 4.696(3) min , IT , 109Pd , 11/2− , , , - , 110Pd , style="text-align:right" , 46 , style="text-align:right" , 64 , 109.905153(12) , colspan=3 align=center, Observationally StableBelieved to decay by ββ to 110Cd with a
half-life Half-life (symbol ) is the time required for a quantity (of substance) to reduce to half of its initial value. The term is commonly used in nuclear physics to describe how quickly unstable atoms undergo radioactive decay or how long stable at ...
over 6×1017 years
, 0+ , 0.1172(9) , , - , 111Pd , style="text-align:right" , 46 , style="text-align:right" , 65 , 110.907671(12) , 23.4(2) min , β , 111mAg , 5/2+ , , , - , rowspan=2 style="text-indent:1em" , 111mPd , rowspan=2 colspan="3" style="text-indent:2em" , 172.18(8) keV , rowspan=2, 5.5(1) h , IT , 111Pd , rowspan=2, 11/2− , rowspan=2, , rowspan=2, , - , β , 111mAg , - , 112Pd , style="text-align:right" , 46 , style="text-align:right" , 66 , 111.907314(19) , 21.03(5) h , β , 112Ag , 0+ , , , - , 113Pd , style="text-align:right" , 46 , style="text-align:right" , 67 , 112.91015(4) , 93(5) s , β , 113mAg , (5/2+) , , , - , style="text-indent:1em" , 113mPd , colspan="3" style="text-indent:2em" , 81.1(3) keV , 0.3(1) s , IT , 113Pd , (9/2−) , , , - , 114Pd , style="text-align:right" , 46 , style="text-align:right" , 68 , 113.910363(25) , 2.42(6) min , β , 114Ag , 0+ , , , - , 115Pd , style="text-align:right" , 46 , style="text-align:right" , 69 , 114.91368(7) , 25(2) s , β , 115mAg , (5/2+)# , , , - , rowspan=2 style="text-indent:1em" , 115mPd , rowspan=2 colspan="3" style="text-indent:2em" , 89.18(25) keV , rowspan=2, 50(3) s , β (92%) , 115Ag , rowspan=2, (11/2−)# , rowspan=2, , rowspan=2, , - , IT (8%) , 115Pd , - , 116Pd , style="text-align:right" , 46 , style="text-align:right" , 70 , 115.91416(6) , 11.8(4) s , β , 116Ag , 0+ , , , - , 117Pd , style="text-align:right" , 46 , style="text-align:right" , 71 , 116.91784(6) , 4.3(3) s , β , 117mAg , (5/2+) , , , - , style="text-indent:1em" , 117mPd , colspan="3" style="text-indent:2em" , 203.2(3) keV , 19.1(7) ms , IT , 117Pd , (11/2−)# , , , - , 118Pd , style="text-align:right" , 46 , style="text-align:right" , 72 , 117.91898(23) , 1.9(1) s , β , 118Ag , 0+ , , , - , 119Pd , style="text-align:right" , 46 , style="text-align:right" , 73 , 118.92311(32)# , 0.92(13) s , β , 119Ag , , , , - , 120Pd , style="text-align:right" , 46 , style="text-align:right" , 74 , 119.92469(13) , 0.5(1) s , β , 120Ag , 0+ , , , - , 121Pd , style="text-align:right" , 46 , style="text-align:right" , 75 , 120.92887(54)# , 285 ms , β , 121Ag , , , , - , 122Pd , style="text-align:right" , 46 , style="text-align:right" , 76 , 121.93055(43)# , 175 ms 300 ns, β , 122Ag , 0+ , , , - , 123Pd , style="text-align:right" , 46 , style="text-align:right" , 77 , 122.93493(64)# , 108 ms , β , 123Ag , , , , - , 124Pd , style="text-align:right" , 46 , style="text-align:right" , 78 , 123.93688(54)# , 38 ms , β , 124Ag , 0+ , , , - , 125Pd , style="text-align:right" , 46 , style="text-align:right" , 79 , , 57 ms , β , 125Ag , , , , - , 126Pd , style="text-align:right" , 46 , style="text-align:right" , 80 , , 48.6 ms , β , 126Ag , 0+ , , , - , style="text-indent:1em" , 126m1Pd , colspan="3" style="text-indent:2em" , 2023 keV , 330 ns , IT , 126Pd , 5− , , , - , style="text-indent:1em" , 126m2Pd , colspan="3" style="text-indent:2em" , 2110 keV , 440 ns , IT , 126m1Pd , 7− , , , - , 127Pd , style="text-align:right" , 46 , style="text-align:right" , 81 , , 38 ms , β , 127Ag , , , , - , 128Pd , style="text-align:right" , 46 , style="text-align:right" , 82 , , 35 ms , β , 128Ag , 0+ , , , - , style="text-indent:1em" , 128mPd , colspan="3" style="text-indent:2em" , 2151 keV , 5.8 µs , IT , 128Pd , 8+ , , , - , 129Pd , style="text-align:right" , 46 , style="text-align:right" , 83 , , 31 ms , β , 129Ag , , ,


Palladium-103

Palladium-103 is a
radioisotope A radionuclide (radioactive nuclide, radioisotope or radioactive isotope) is a nuclide that has excess nuclear energy, making it unstable. This excess energy can be used in one of three ways: emitted from the nucleus as gamma radiation; transferr ...
of the element
palladium Palladium is a chemical element with the symbol Pd and atomic number 46. It is a rare and lustrous silvery-white metal discovered in 1803 by the English chemist William Hyde Wollaston. He named it after the asteroid Pallas, which was itself na ...
that has uses in
radiation therapy Radiation therapy or radiotherapy, often abbreviated RT, RTx, or XRT, is a therapy using ionizing radiation, generally provided as part of cancer treatment to control or kill malignant cells and normally delivered by a linear accelerator. Radi ...
for prostate cancer and
uveal melanoma Uveal melanoma is a type of eye cancer in the uvea of the eye. It is traditionally classed as originating in the iris, choroid, and ciliary body, but can also be divided into class I (low metastatic risk) and class II (high metastatic risk). Sym ...
. Palladium-103 may be created from palladium-102 or from rhodium-103 using a
cyclotron A cyclotron is a type of particle accelerator invented by Ernest O. Lawrence in 1929–1930 at the University of California, Berkeley, and patented in 1932. Lawrence, Ernest O. ''Method and apparatus for the acceleration of ions'', filed: Jan ...
. Palladium-103 has a
half-life Half-life (symbol ) is the time required for a quantity (of substance) to reduce to half of its initial value. The term is commonly used in nuclear physics to describe how quickly unstable atoms undergo radioactive decay or how long stable at ...
of 16.99 days and decays by
electron capture Electron capture (K-electron capture, also K-capture, or L-electron capture, L-capture) is a process in which the proton-rich nucleus of an electrically neutral atom absorbs an inner atomic electron, usually from the K or L electron shells. Thi ...
to rhodium-103, emitting characteristic
x-ray An X-ray, or, much less commonly, X-radiation, is a penetrating form of high-energy electromagnetic radiation. Most X-rays have a wavelength ranging from 10  picometers to 10  nanometers, corresponding to frequencies in the range 30&nb ...
s with 21
keV Kev can refer to: Given name * Kev Adams, French comedian, actor, screenwriter and film producer born Kevin Smadja in 1991 * Kevin Kev Carmody (born 1946), Indigenous Australian singer-songwriter * Kev Coghlan (born 1988), Scottish Grand Prix moto ...
of
energy In physics, energy (from Ancient Greek: ἐνέργεια, ''enérgeia'', “activity”) is the quantitative property that is transferred to a body or to a physical system, recognizable in the performance of work and in the form of hea ...
.


Palladium-107

Palladium-107 is the second-longest lived (
half-life Half-life (symbol ) is the time required for a quantity (of substance) to reduce to half of its initial value. The term is commonly used in nuclear physics to describe how quickly unstable atoms undergo radioactive decay or how long stable at ...
of 6.5 million years) and least radioactive (
decay energy The decay energy is the energy change of a nucleus having undergone a radioactive decay. Radioactive decay is the process in which an unstable atomic nucleus loses energy by emitting ionizing particles and radiation. This decay, or loss of energy ...
only 33 
keV Kev can refer to: Given name * Kev Adams, French comedian, actor, screenwriter and film producer born Kevin Smadja in 1991 * Kevin Kev Carmody (born 1946), Indigenous Australian singer-songwriter * Kev Coghlan (born 1988), Scottish Grand Prix moto ...
,
specific activity Specific activity is the activity per unit mass of a radionuclide and is a physical property of that radionuclide. Activity is a quantity (for which the SI unit is the becquerel) related to radioactivity, and is defined as the number of radi ...
5 Ci/g) of the 7 long-lived fission products. It undergoes pure
beta decay In nuclear physics, beta decay (β-decay) is a type of radioactive decay in which a beta particle (fast energetic electron or positron) is emitted from an atomic nucleus, transforming the original nuclide to an isobar of that nuclide. For ...
(without gamma radiation) to 107Ag, which is stable. Its yield from
thermal neutron The neutron detection temperature, also called the neutron energy, indicates a free neutron's kinetic energy, usually given in electron volts. The term ''temperature'' is used, since hot, thermal and cold neutrons are moderated in a medium wi ...
fission of
uranium-235 Uranium-235 (235U or U-235) is an isotope of uranium making up about 0.72% of natural uranium. Unlike the predominant isotope uranium-238, it is fissile, i.e., it can sustain a nuclear chain reaction. It is the only fissile isotope that exi ...
is 0.1629% per fission, only 1/4 that of
iodine-129 Iodine-129 (129I) is a long-lived radioisotope of iodine which occurs naturally, but also is of special interest in the monitoring and effects of man-made nuclear fission products, where it serves as both tracer and potential radiological contamin ...
, and only 1/40 those of 99Tc, 93Zr, and 135Cs. Yield from 233U is slightly lower, but yield from 239Pu is much higher, 3.3%.
Fast fission Fast fission is fission that occurs when a heavy atom absorbs a high-energy neutron, called a fast neutron, and splits. Most fissionable materials need thermal neutrons, which move more slowly. Fast reactors vs. thermal reactors Fast neutron re ...
or fission of some heavier
actinides The actinide () or actinoid () series encompasses the 15 metallic chemical elements with atomic numbers from 89 to 103, actinium through lawrencium. The actinide series derives its name from the first element in the series, actinium. The inform ...
'' hich?' will produce palladium-107 at higher yields. One source estimates that palladium produced from fission contains the isotopes 104Pd (16.9%),105Pd (29.3%), 106Pd (21.3%), 107Pd (17%), 108Pd (11.7%) and 110Pd (3.8%). According to another source, the proportion of 107Pd is 9.2% for palladium from thermal neutron fission of 235U, 11.8% for 233U, and 20.4% for 239Pu (and the 239Pu yield of palladium is about 10 times that of 235U). Because of this dilution and because 105Pd has 11 times the
neutron absorption Neutron capture is a nuclear reaction in which an atomic nucleus and one or more neutrons collide and merge to form a heavier nucleus. Since neutrons have no electric charge, they can enter a nucleus more easily than positively charged protons, ...
cross section Cross section may refer to: * Cross section (geometry) ** Cross-sectional views in architecture & engineering 3D *Cross section (geology) * Cross section (electronics) * Radar cross section, measure of detectability * Cross section (physics) **Abs ...
, 107Pd is not amenable to disposal by nuclear transmutation. However, as a
noble metal A noble metal is ordinarily regarded as a metallic chemical element that is generally resistant to corrosion and is usually found in nature in its raw form. Gold, platinum, and the other platinum group metals ( ruthenium, rhodium, palladium, o ...
, palladium is not as mobile in the environment as iodine or technetium.


References


Patent application for Palladium-103 implantable radiation-delivery device
(accessed 12/7/05) * Isotope masses from: ** * Isotopic compositions and standard atomic masses from: ** ** * Half-life, spin, and isomer data selected from the following sources. ** ** ** {{Navbox element isotopes Palladium
Palladium Palladium is a chemical element with the symbol Pd and atomic number 46. It is a rare and lustrous silvery-white metal discovered in 1803 by the English chemist William Hyde Wollaston. He named it after the asteroid Pallas, which was itself na ...