K line is a term used in Internal conversion electron spectroscopy.

A new detector system has been developed at the Department to study conversion electrons emitted in the decay of extreme nuclear states.

The Chalk River -spectrometer was used to select the conversion electrons.

Conversion electrons from the decay of 134Cs have been investigated using a mini-orange electron spectrometer.

The conversion electrons from these decays are investigated using a mini-orange electron spectrometer.

Internal conversion electrons accompanying slow neutron capture in Gd.

The germanium isotope emits two weak gamma rays and a conversion electron.

Only the further search for characteristic X-rays and conversion electron signals resulted in the identification of a berkelium isotope.

Most nuclear excited states decay by gamma ray emission or conversion electron, though, far from stability, other decay modes are known.

The nucleus will eventually relax (i.e., de-excite) to its ground state through the emission of gamma rays or internal conversion electrons.

A nucleus thus produced generally starts its existence in an excited state that relaxes through the emission of one or more gamma rays or conversion electrons.

A much smaller dose would be absorbed from the penetrating X- and γ-rays and internal conversion electrons released from other radiolabelled cells in the culture.

A material that spontaneously emits such radiation - which includes alpha particles, beta particles, gamma rays and conversion electrons - is considered radioactive.

In this paper we have calculated an expression for the probability of capture of atomic, low-energy conversion electrons by Davydov's solitons, the atom being attached to a one-dimensional molecular crystal.

These conversion electrons will ionize the surrounding matter like beta radiation electrons would do, contributing along with the 140.5 keV and 142.6 keV gammas to the total deposited dose.

Gamma radiation and conversion electrons following the reaction 169Tm(α,2n)171Lu have been studied, using high resolution Ge(Li) detectors in singles and coincidence mode, and an on-line, double-focussing, electron spectrometer.

The electron capture produces a tellurium-125 nucleus in an excited state with a half-life of 1.6 ns, which undergoes gamma decay emitting a photon or an internal conversion electron at 35.5 keV.

Conversion electron mössbauer spectroscopy (CEMS) is a Mössbauer spectroscopy technique based on conversion electron.

The damage from the more penetrating gamma radiation and 127 keV internal conversion electron radiation from the initial decay of Te-123 is moderated by the relatively short half-life of the isotope.

The L2 and L3 subshell fluorescence yields, ω2 and ω3, and the Coster–Kronig transition probability f23 in 88Ra and 94Pu have been deduced from conversion electron L X-ray coincidence measurements.

Excited Te-125 from EC decay of I-125 also emits a much lower-energy internal conversion electron (35.5 keV), which does relatively little damage due to its low energy, even though its emission is more common.

The gamma rays, beta rays, and conversion electrons emitted in the beta decay of 124Sb → 124Te have been observed using Ge(Li) and Si(Li) detectors both singly and in coincidence.

The conversion electron intensities for the transitions with energy above 800 keV from the 182Ta decay were measured using a mini-orange electron spectrometer and the internal conversion coefficients for various transitions in 182W deduced.

Following EC, the excited Te-123 from I-123 emits a high-speed 127 keV internal conversion electron (not a beta ray) about 13% of the time, but this does little cellular damage due to the nuclide's short half-life and the relatively small fraction of such events.

As an atom may produce an internal conversion electron in place of a gamma ray, an atom may produce an Auger electron in place of an x ray if an electron is missing from one of the electron shells.