Annika Lohstroh

Annika Lohstroh


Research Focus & Metrics

Academic Career Length

26Years (2001-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 December 2005 in IEEE Transactions on Nuclear Science
Verified
Journal Article
Closed access
PSPaul Sellin
Paul Sellin
ADA.W. Davies
A.W. Davies
ALAnnika Lohstroh
Annika Lohstroh
MOM.E. Ozsan
M.E. Ozsan
JPJ. Parkin
J. Parkin
We report the electron and hole charge transport properties of semi insulating CdTe:Cl grown by the Travelling Heater Method (THM). An alpha-particle Time of Flight (TOF) method was used to measure electron and hole drift mobility, with room temperature values of 880 cm2 /Vs for electrons and 90 cm2/Vs for holes. The variation in mobility was also investigated as a function of temperature, with electron and hole mobilities at 190 K of 1150 cm2 /Vs and 20 cm2/Vs respectively. Using a Hecht analysis the electron and hole mobility-lifetime products were also measured over the same temperature range, with values at room temperature of 8times10-4 cm2/V and 7times10-5 cm 2/V respectively. Time-resolved ion beam induced charge (IBIC) imaging was used to produce micrometer resolution maps of electron drift mobility and signal amplitude, which showed excellent spatial uniformity

5 March 2007 in Applied Physics Letters
Verified
Journal Article
Closed access
PDF file
ALAnnika Lohstroh
Annika Lohstroh
PSPaul Sellin
Paul Sellin
SWS. G. Wang
S. G. Wang
ADA. W. Davies
A. W. Davies
JPJ. Parkin
J. Parkin
Paul R. EdwardsPaul R. Edwards
Paul R. Edwards
The authors report correlations between variations in charge transport of electrons and holes in synthetic single crystal diamond and the presence of nitrogen impurities and dislocations. The spatial distribution of these defects was imaged using their characteristic luminescence emission and compared with maps of carrier drift length measured by ion beam induced charge imaging. The images indicate a reduction of electron and hole mobility–lifetime product due to nitrogen impurities and dislocations. Very good charge transport is achieved in selected regions where the dislocation density is minimal.

1 April 2008 in Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
Verified
Journal Article
Closed access
PSPaul Sellin
Paul Sellin
ADA.W. Davies
A.W. Davies
SGS. Gkoumas
S. Gkoumas
ALAnnika Lohstroh
Annika Lohstroh
MÖM.E. Özsan
M.E. Özsan
Matthew VealeMatthew Veale
Matthew Veale

1 January 2011 in Reviews of Accelerator Science and Technology
Verified
Journal Article
Closed access
CJChris Jeynes
Chris Jeynes
RWRoger P. Webb
Roger P. Webb
ALAnnika Lohstroh
Annika Lohstroh

15 March 2007 in Journal of Applied Physics
Verified
Journal Article
Closed access
PDF file
ALAnnika Lohstroh
Annika Lohstroh
PSPaul Sellin
Paul Sellin
SWS. G. Wang
S. G. Wang
ADA. W. Davies
A. W. Davies
JPJ. M. Parkin
J. M. Parkin
Diamond has been regarded as a promising radiation detector material for use as a solid state ionizing chamber for decades. The parameters degrading the charge transport from what is expected from an ideal crystal are still not completely understood. Recently, synthetic chemical vapor deposited (CVD) single crystal diamond has become available, offering the opportunity to study the properties of synthesized material independent of grain boundaries. We have studied the charge transport of a synthetic single crystal diamond with α -particle induced charge transients as a function of temperature and established the presence of a shallow hole trap with an activation energy of 0.29±0.02eV in some parts of the detector. Ion beam induced charge imaging has been used to study the spatial variations of the charge transport in a synthetic single crystal diamond. Pulses influenced by the shallow hole trap had their origin close to the substrate∕CVD interface of the sample. They could be clearly distinguished from pulses affected by reduced charge carrier velocities due to polarization phenomena, which varied systematically with the growth direction of the CVD diamond material.