
Ion Time-of-Flight Spectrometer
Development of an Ion Time-of-Flight Spectrometer for Neutron Depth Profiling
Versandkostenfrei!
Versandfertig in 6-10 Tagen
52,99 €
inkl. MwSt.
PAYBACK Punkte
26 °P sammeln!
Ion time-of-flight spectrometry techniques are investigated for potential application to neutron depth profiling. Time-of-flight techniques are used extensively in a wide range of scientific and technological applications including energy and mass spectroscopy. Ion time-of-flight spectrometry offers highly precise measurement capabilities, particularly for slow particles. Time-of-flight spectrometry involves correlated detection of two signals by a coincidence unit. In ion time-of-flight spectroscopy, the ion generates the primary input signal. The secondary signal can be obtained by a number ...
Ion time-of-flight spectrometry techniques are
investigated for potential application to neutron
depth profiling. Time-of-flight techniques are used
extensively in a wide range of scientific and
technological applications including energy and mass
spectroscopy. Ion time-of-flight spectrometry offers
highly precise measurement capabilities, particularly
for slow particles. Time-of-flight spectrometry
involves correlated detection of two signals by a
coincidence unit. In ion time-of-flight spectroscopy,
the ion generates the primary input signal. The
secondary signal can be obtained by a number of ways.
In this work, the secondary signal is created by the
passage of the primary ion through a thin carbon
foil. Two ion time-of-flight spectrometer design
paradigms are introduced: the parallel electric and
magnetic (PEM) field spectrometer and the cross
electric and magnetic (CEM) field spectrometer.
investigated for potential application to neutron
depth profiling. Time-of-flight techniques are used
extensively in a wide range of scientific and
technological applications including energy and mass
spectroscopy. Ion time-of-flight spectrometry offers
highly precise measurement capabilities, particularly
for slow particles. Time-of-flight spectrometry
involves correlated detection of two signals by a
coincidence unit. In ion time-of-flight spectroscopy,
the ion generates the primary input signal. The
secondary signal can be obtained by a number of ways.
In this work, the secondary signal is created by the
passage of the primary ion through a thin carbon
foil. Two ion time-of-flight spectrometer design
paradigms are introduced: the parallel electric and
magnetic (PEM) field spectrometer and the cross
electric and magnetic (CEM) field spectrometer.