Isotopes of praseodymium
Encyclopedia
Naturally occurring praseodymium
(Pr) is composed of one stable isotope
, 141Pr. Thirty-eight radioisotopes have been characterized with the most stable being 143Pr with a half-life
of 13.57 days and 142Pr with a half-life of 19.12 hours. All of the remaining radioactive isotopes have half-lives that are less than 5.985 hours and the majority of these have half-lives that are less than 33 seconds. This element also has 15 meta states with the most stable being 138mPr (t½ 2.12 hours), 142mPr (t½ 14.6 minutes) and 134mPr (t½ 11 minutes).
The isotopes of praseodymium range in atomic weight
from 120.955 u
(121Pr) to 158.955 u (159Pr). The primary decay mode before the stable isotope, 141Pr, is electron capture
and the primary mode after is beta minus decay. The primary decay product
s before 141Pr are element 58 (cerium
) isotopes and the primary products after are element 60 (neodymium
) isotopes.
Standard atomic mass: 140.90765(2) u
Praseodymium
Praseodymium is a chemical element that has the symbol Pr and atomic number 59. Praseodymium is a soft, silvery, malleable and ductile metal in the lanthanide group. It is too reactive to be found in native form, and when artificially prepared, it slowly develops a green oxide coating.The element...
(Pr) is composed of one stable isotope
Isotope
Isotopes are variants of atoms of a particular chemical element, which have differing numbers of neutrons. Atoms of a particular element by definition must contain the same number of protons but may have a distinct number of neutrons which differs from atom to atom, without changing the designation...
, 141Pr. Thirty-eight radioisotopes have been characterized with the most stable being 143Pr with a half-life
Half-life
Half-life, abbreviated t½, is the period of time it takes for the amount of a substance undergoing decay to decrease by half. The name was originally used to describe a characteristic of unstable atoms , but it may apply to any quantity which follows a set-rate decay.The original term, dating to...
of 13.57 days and 142Pr with a half-life of 19.12 hours. All of the remaining radioactive isotopes have half-lives that are less than 5.985 hours and the majority of these have half-lives that are less than 33 seconds. This element also has 15 meta states with the most stable being 138mPr (t½ 2.12 hours), 142mPr (t½ 14.6 minutes) and 134mPr (t½ 11 minutes).
The isotopes of praseodymium range in atomic weight
Atomic weight
Atomic weight is a dimensionless physical quantity, the ratio of the average mass of atoms of an element to 1/12 of the mass of an atom of carbon-12...
from 120.955 u
Atomic mass unit
The unified atomic mass unit or dalton is a unit that is used for indicating mass on an atomic or molecular scale. It is defined as one twelfth of the rest mass of an unbound neutral atom of carbon-12 in its nuclear and electronic ground state, and has a value of...
(121Pr) to 158.955 u (159Pr). The primary decay mode before the stable isotope, 141Pr, is electron capture
Electron capture
Electron capture is a process in which a proton-rich nuclide absorbs an inner atomic electron and simultaneously emits a neutrino...
and the primary mode after is beta minus decay. The primary decay product
Decay product
In nuclear physics, a decay product is the remaining nuclide left over from radioactive decay. Radioactive decay often involves a sequence of steps...
s before 141Pr are element 58 (cerium
Cerium
Cerium is a chemical element with the symbol Ce and atomic number 58. It is a soft, silvery, ductile metal which easily oxidizes in air. Cerium was named after the dwarf planet . Cerium is the most abundant of the rare earth elements, making up about 0.0046% of the Earth's crust by weight...
) isotopes and the primary products after are element 60 (neodymium
Neodymium
Neodymium is a chemical element with the symbol Nd and atomic number 60. It is a soft silvery metal that tarnishes in air. Neodymium was discovered in 1885 by the Austrian chemist Carl Auer von Welsbach. It is present in significant quantities in the ore minerals monazite and bastnäsite...
) isotopes.
Standard atomic mass: 140.90765(2) u
Table
nuclide symbol |
Z(p Proton The proton is a subatomic particle with the symbol or and a positive electric charge of 1 elementary charge. One or more protons are present in the nucleus of each atom, along with neutrons. The number of protons in each atom is its atomic number.... ) |
N(n Neutron The neutron is a subatomic hadron particle which has the symbol or , no net electric charge and a mass slightly larger than that of a proton. With the exception of hydrogen, nuclei of atoms consist of protons and neutrons, which are therefore collectively referred to as nucleons. The number of... ) |
isotopic mass (u) |
half-life | decay mode(s)Abbreviations: EC: Electron capture Electron capture Electron capture is a process in which a proton-rich nuclide absorbs an inner atomic electron and simultaneously emits a neutrino... IT: Isomeric transition Isomeric transition An isomeric transition is a radioactive decay process that involves emission of a gamma ray from an atom where the nucleus is in an excited metastable state, referred to in its excited state, as a nuclear isomer.... |
daughter isotope(s)Bold for stable isotopes, bold italics for nearly-stable isotopes (half-life longer than the age of the universe Age of the universe The age of the universe is the time elapsed since the Big Bang posited by the most widely accepted scientific model of cosmology. The best current estimate of the age of the universe is 13.75 ± 0.13 billion years within the Lambda-CDM concordance model... ) |
nuclear spin |
representative isotopic composition (mole fraction) |
range of natural variation (mole fraction) |
---|---|---|---|---|---|---|---|---|---|
excitation energy | |||||||||
121Pr | 59 | 62 | 120.95536(75)# | 600(300) ms | p Proton emission Proton emission is a type of radioactive decay in which a proton is ejected from a nucleus. Proton emission can occur from high-lying excited states in a nucleus following a beta decay, in which case the process is known as beta-delayed proton emission, or can occur from the ground state of very... |
120Ce | (3/2-) | ||
β+ Beta decay In nuclear physics, beta decay is a type of radioactive decay in which a beta particle is emitted from an atom. There are two types of beta decay: beta minus and beta plus. In the case of beta decay that produces an electron emission, it is referred to as beta minus , while in the case of a... (rare) |
121Ce | ||||||||
β+, p (rare) | 120La | ||||||||
122Pr | 59 | 63 | 121.95181(54)# | 500# ms | β+ | 122Ce | |||
123Pr | 59 | 64 | 122.94596(64)# | 800# ms | β+ | 123Ce | 3/2+# | ||
124Pr | 59 | 65 | 123.94296(64)# | 1.2(2) s | β+ | 124Ce | |||
β+, p (rare) | 123La | ||||||||
125Pr | 59 | 66 | 124.93783(43)# | 3.3(7) s | β+ | 125Ce | 3/2+# | ||
β+, p (rare) | 124La | ||||||||
126Pr | 59 | 67 | 125.93531(21)# | 3.12(18) s | β+ | 126Ce | (4,5,6) | ||
β+, p (rare) | 125La | ||||||||
127Pr | 59 | 68 | 126.93083(21)# | 4.2(3) s | β+ | 127Ce | 3/2+# | ||
127mPr | 600(200)# keV | 50# ms | 11/2- | ||||||
128Pr | 59 | 69 | 127.92879(3) | 2.84(9) s | β+ | 128Ce | (3+) | ||
β+, p (rare) | 127La | ||||||||
129Pr | 59 | 70 | 128.92510(3) | 32(3) s | β+ | 129Ce | (11/2-) | ||
129mPr | 382.7(5) keV | 1# ms | β+ | 129Ce | (11/2-) | ||||
130Pr | 59 | 71 | 129.92359(7) | 40.0(4) s | β+ | 130Ce | (6,7)(+#) | ||
130mPr | 100(100)# keV | 10# s | 2+# | ||||||
131Pr | 59 | 72 | 130.92026(6) | 1.50(3) min | β+ | 131Ce | (3/2+) | ||
131mPr | 152.4(2) keV | 5.7(2) s | IT Isomeric transition An isomeric transition is a radioactive decay process that involves emission of a gamma ray from an atom where the nucleus is in an excited metastable state, referred to in its excited state, as a nuclear isomer.... (96.4%) |
131Pr | (11/2-) | ||||
β+ (3.59%) | 131Ce | ||||||||
132Pr | 59 | 73 | 131.91926(6) | 1.49(11) min | β+ | 132Ce | (2+) | ||
132mPr | 0(100)# keV | 20# s | β+ | 132Ce | (5+) | ||||
133Pr | 59 | 74 | 132.916331(13) | 6.5(3) min | β+ | 133Ce | (3/2+) | ||
133mPr | 192.05(14) keV | 1.1(2) µs | (11/2-) | ||||||
134Pr | 59 | 75 | 133.91571(4) | ~11 min | β+ | 134Ce | (5-) | ||
134mPr | 0(100)# keV | 17(2) min | β+ | 134Ce | 2- | ||||
135Pr | 59 | 76 | 134.913112(13) | 24(2) min | β+ | 135Ce | 3/2(+) | ||
135mPr | 358.06(6) keV | 105(10) µs | (11/2-) | ||||||
136Pr | 59 | 77 | 135.912692(13) | 13.1(1) min | β+ | 136Ce | 2+ | ||
137Pr | 59 | 78 | 136.910705(13) | 1.28(3) h | β+ | 137Ce | 5/2+ | ||
137mPr | 561.22(23) keV | 2.66(7) µs | 11/2- | ||||||
138Pr | 59 | 79 | 137.910755(15) | 1.45(5) min | β+ | 138Ce | 1+ | ||
138mPr | 348(23) keV | 2.12(4) h | β+ | 138Ce | 7- | ||||
139Pr | 59 | 80 | 138.908938(8) | 4.41(4) h | β+ | 139Ce | 5/2+ | ||
140Pr | 59 | 81 | 139.909076(7) | 3.39(1) min | β+ | 140Ce | 1+ | ||
140m1Pr | 127.5(3) keV | 0.35(2) µs | 5+ | ||||||
140m2Pr | 763.3(7) keV | 3.05(20) µs | (8)- | ||||||
141PrFission product Fission product Nuclear fission products are the atomic fragments left after a large atomic nucleus fissions. Typically, a large nucleus like that of uranium fissions by splitting into two smaller nuclei, along with a few neutrons and a large release of energy in the form of heat , gamma rays and neutrinos. The... |
59 | 82 | 140.9076528(26) | Observationally StableTheoretically capable of spontaneous fission Spontaneous fission Spontaneous fission is a form of radioactive decay characteristic of very heavy isotopes. Because the nuclear binding energy reaches a maximum at a nuclear mass greater than about 60 atomic mass units , spontaneous breakdown into smaller nuclei and single particles becomes possible at heavier masses... |
5/2+ | 1.0000 | |||
142Pr | 59 | 83 | 141.9100448(26) | 19.12(4) h | β- (99.98%) | 142Nd | 2- | ||
EC Electron capture Electron capture is a process in which a proton-rich nuclide absorbs an inner atomic electron and simultaneously emits a neutrino... (.0164%) |
142Ce | ||||||||
142mPr | 3.694(3) keV | 14.6(5) min | IT | 142Pr | 5- | ||||
143Pr | 59 | 84 | 142.9108169(28) | 13.57(2) d | β- | 143Nd | 7/2+ | ||
144Pr | 59 | 85 | 143.913305(4) | 17.28(5) min | β- | 144Nd | 0- | ||
144mPr | 59.03(3) keV | 7.2(3) min | IT (99.93%) | 144Pr | 3- | ||||
β- (.07%) | 144Nd | ||||||||
145Pr | 59 | 86 | 144.914512(8) | 5.984(10) h | β- | 145Nd | 7/2+ | ||
146Pr | 59 | 87 | 145.91764(7) | 24.15(18) min | β- | 146Nd | (2)- | ||
147Pr | 59 | 88 | 146.918996(25) | 13.4(4) min | β- | 147Nd | (3/2+) | ||
148Pr | 59 | 89 | 147.922135(28) | 2.29(2) min | β- | 148Nd | 1- | ||
148mPr | 50(30)# keV | 2.01(7) min | β- | 148Nd | (4) | ||||
149Pr | 59 | 90 | 148.92372(9) | 2.26(7) min | β- | 149Nd | (5/2+) | ||
150Pr | 59 | 91 | 149.926673(28) | 6.19(16) s | β- | 150Nd | (1)- | ||
151Pr | 59 | 92 | 150.928319(25) | 18.90(7) s | β- | 151Nd | (3/2)(-#) | ||
152Pr | 59 | 93 | 151.93150(13) | 3.63(12) s | β- | 152Nd | 4+ | ||
153Pr | 59 | 94 | 152.93384(11) | 4.28(11) s | β- | 153Nd | 5/2-# | ||
154Pr | 59 | 95 | 153.93752(16) | 2.3(1) s | β- | 154Nd | (3+,2+) | ||
155Pr | 59 | 96 | 154.94012(32)# | 1# s [>300 ns] | β- | 155Nd | 5/2-# | ||
156Pr | 59 | 97 | 155.94427(43)# | 500# ms [>300 ns] | β- | 156Nd | |||
157Pr | 59 | 98 | 156.94743(43)# | 300# ms | β- | 157Nd | 5/2-# | ||
158Pr | 59 | 99 | 157.95198(64)# | 200# ms | β- | 158Nd | |||
159Pr | 59 | 100 | 158.95550(75)# | 100# ms | β- | 159Nd | 5/2-# |