Isotopes of lawrencium
Encyclopedia
Lawrencium
(Lr) is an artificial element, and thus a standard atomic mass
cannot be given. Like all artificial elements, it has no stable isotope
s. The first isotope
to be synthesized was 258Lr in 1961. There are eleven known radioisotopes from 252Lr to 262Lr, and 1 isomer
(253mLr). The longest-lived isotope is 262Lr with a half-life
of 216 minutes. Heavier isotopes are expected to have longer half-lives.
Lawrencium
Lawrencium is a radioactive synthetic chemical element with the symbol Lr and atomic number 103. In the periodic table of the elements, it is a period 7 d-block element and the last element of actinide series...
(Lr) is an artificial element, and thus a standard atomic mass
Atomic mass
The atomic mass is the mass of a specific isotope, most often expressed in unified atomic mass units. The atomic mass is the total mass of protons, neutrons and electrons in a single atom....
cannot be given. Like all artificial elements, it has no stable isotope
Stable isotope
Stable isotopes are chemical isotopes that may or may not be radioactive, but if radioactive, have half-lives too long to be measured.Only 90 nuclides from the first 40 elements are energetically stable to any kind of decay save proton decay, in theory...
s. The first 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...
to be synthesized was 258Lr in 1961. There are eleven known radioisotopes from 252Lr to 262Lr, and 1 isomer
Nuclear isomer
A nuclear isomer is a metastable state of an atomic nucleus caused by the excitation of one or more of its nucleons . "Metastable" refers to the fact that these excited states have half-lives more than 100 to 1000 times the half-lives of the other possible excited nuclear states...
(253mLr). The longest-lived isotope is 262Lr 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 216 minutes. Heavier isotopes are expected to have longer half-lives.
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: SF: 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... |
daughter isotope(s) |
nuclear spin |
|---|---|---|---|---|---|---|---|
| excitation energy | |||||||
| 252LrNot directly synthesized, occurs as a 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... of 256Db |
103 | 149 | 252.09537(27)# | 390(90) ms [0.36(+11-7) s] |
α Alpha decay Alpha decay is a type of radioactive decay in which an atomic nucleus emits an alpha particle and thereby transforms into an atom with a mass number 4 less and atomic number 2 less... (90%) |
248Md | |
| 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... (10%) |
252No | ||||||
| SF 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... (1%) |
(various) | ||||||
| 253LrNot directly synthesized, occurs as a decay product of 257Db | 103 | 150 | 253.09521(24)# | 580(70) ms [0.57(+7-6) s] |
α (90%) | 249Md | (7/2-) |
| SF (9%) | (various) | ||||||
| β+ (1%) | 253No | ||||||
| 253mLr | 30(100)# keV | 1.5(3) s [1.5(+3-2) s] |
(1/2-) | ||||
| 254LrNot directly synthesized, occurs as a decay product of 258Db | 103 | 151 | 254.09645(36)# | 13(3) s | α (78%) | 250Md | |
| β+ (22%) | 254No | ||||||
| SF (.1%) | (various) | ||||||
| 255Lr | 103 | 152 | 255.09668(22)# | 22(4) s | α (69%) | 251Md | 7/2-# |
| β+ (30%) | 255No | ||||||
| SF (1%) | (various) | ||||||
| 256Lr | 103 | 153 | 256.09863(24)# | 27(3) s | α (80%) | 252Md | |
| β+ (20%) | 256No | ||||||
| SF (.01%) | (various) | ||||||
| 257Lr | 103 | 154 | 257.09956(22)# | 646(25) ms | α (99.99%) | 253Md | 9/2+# |
| β+ (.01%) | 257No | ||||||
| SF (.001%) | (various) | ||||||
| 258Lr | 103 | 155 | 258.10181(11)# | 4.1(3) s | α (95%) | 254Md | |
| β+ (5%) | 258No | ||||||
| 259Lr | 103 | 156 | 259.10290(8)# | 6.2(3) s | α (77%) | 255Md | 9/2+# |
| SF (23%) | (various) | ||||||
| β+ (.5%) | 259No | ||||||
| 260Lr | 103 | 157 | 260.10550(12)# | 2.7 min | α (75%) | 256Md | |
| β+ (15%) | 260No | ||||||
| SF (10%) | (various) | ||||||
| 261Lr | 103 | 158 | 261.10688(22)# | 44 min | SF | (various) | |
| α (rare) | 257Md | ||||||
| 262Lr | 103 | 159 | 262.10963(22)# | 216 min | β+ | 262No | |
| α (rare) | 258Md | ||||||