Adam E. Hansen

Adam E. Hansen

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Research Focus & Metrics

Academic Career Length

31Years (1996-Present)

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

Representative Publications

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28 July 2004 in Nano Letters
Verified
Journal Article
Closed access
MBMikael T. Björk
Mikael T. Björk
CTClaes Thelander
Claes Thelander
AHAdam E. Hansen
Adam E. Hansen
LJLinus E. Jensen
Linus E. Jensen
MLMagnus W. Larsson
Magnus W. Larsson
LSLars Samuelson
Lars Samuelson

28 October 2010 in Annals of Neurology
Verified
Journal Article
Closed access
PDF file
MAMohammad S. Asghar
Mohammad S. Asghar
AHAdam E. Hansen
Adam E. Hansen
FAFaisal Mohammad Amin
Faisal Mohammad Amin
RGR. J. van der Geest
R. J. van der Geest
PKPatrick van der Koning
Patrick van der Koning
MAMessoud Ashina
Messoud Ashina

1 May 2013 in The Lancet Neurology
Verified
Journal Article
Closed access
FAFaisal Mohammad Amin
Faisal Mohammad Amin
MAMohammad Sohail Asghar
Mohammad Sohail Asghar
AHAnders Hougaard
Anders Hougaard
AHAdam E. Hansen
Adam E. Hansen
VLVibeke Andrée Larsen
Vibeke Andrée Larsen
MAMessoud Ashina
Messoud Ashina

1 May 2014 in NeuroImage
Verified
Journal Article
Closed access
DGDouglas N. Greve
Douglas N. Greve
CSClaus Svarer
Claus Svarer
PFPatrick M. Fisher
Patrick M. Fisher
LFLing Feng
Ling Feng
AHAdam E. Hansen
Adam E. Hansen
GKGitte Moos Knudsen
Gitte Moos Knudsen

15 October 2000 in Physical Review B
Verified
Journal Article
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AKAnders Kristensen
Anders Kristensen
Henrik BruusHenrik Bruus
Henrik Bruus
AHAdam E. Hansen
Adam E. Hansen
JJJ. B. Jensen
J. B. Jensen
PLP. E. Lindelof
P. E. Lindelof
MMM. Michel
M. Michel
The 0.7(2e2/h) conductance anomaly is studied in strongly confined, etched GaAs/GaAlAs quantum point contacts, by measuring the differential conductance as a function of source-drain and gate bias as well as a function of temperature. We investigate in detail how, for a given gate voltage, the differential conductance depends on the finite bias voltage and find a so-called self-gating effect, which we correct for. The 0.7 anomaly at zero bias is found to evolve smoothly into a conductance plateau at 0.85(2e2/h) at finite bias. On varying the gate voltage the transition between the 1.0 and 0.85(2e2/h) plateaus occurs for definite bias voltages, which define a gate-voltage-dependent energy difference Δ. This energy difference is compared with the activation temperature Ta extracted from the experimentally observed activated behavior of the 0.7 anomaly at low bias. We find Δ=kBTa, which lends support to the idea that the conductance anomaly is due to transmission through two conduction channels, of which the one with its subband edge Δ below the chemical potential becomes thermally depopulated as the temperature is increased.

1 February 2017 in NeuroImage
Verified
Journal Article
Open access
CLClaes N. Ladefoged
Claes N. Ladefoged
ILIan Law
Ian Law
UAUdunna Anazodo
Udunna Anazodo
KLKeith St. Lawrence
Keith St. Lawrence
DGDavid Izquierdo Garcia
David Izquierdo Garcia
FAFlemming Littrup Andersen
Flemming Littrup Andersen
To accurately quantify the radioactivity concentration measured by PET, emission data need to be corrected for photon attenuation; however, the MRI signal cannot easily be converted into attenuation values, making attenuation correction (AC) in PET/MRI challenging. In order to further improve the current vendor-implemented MR-AC methods for absolute quantification, a number of prototype methods have been proposed in the literature. These can be categorized into three types: template/atlas-based, segmentation-based, and reconstruction-based. These proposed methods in general demonstrated improvements compared to vendor-implemented AC, and many studies report deviations in PET uptake after AC of only a few percent from a gold standard CT-AC. Using a unified quantitative evaluation with identical metrics, subject cohort, and common CT-based reference, the aims of this study were to evaluate a selection of novel methods proposed in the literature, and identify the ones suitable for clinical use. In total, 11 AC methods were evaluated: two vendor-implemented (MR-ACDIXON and MR-ACUTE), five based on template/atlas information (MR-ACSEGBONE (Koesters et al., 2016), MR-ACONTARIO (Anazodo et al., 2014), MR-ACBOSTON (Izquierdo-Garcia et al., 2014), MR-ACUCL (Burgos et al., 2014), and MR-ACMAXPROB (Merida et al., 2015)), one based on simultaneous reconstruction of attenuation and emission (MR-ACMLAA (Benoit et al., 2015)), and three based on image-segmentation (MR-ACMUNICH (Cabello et al., 2015), MR-ACCAR-RiDR (Juttukonda et al., 2015), and MR-ACRESOLUTE (Ladefoged et al., 2015)). We selected 359 subjects who were scanned using one of the following radiotracers: [18F]FDG (210), [11C]PiB (51), and [18F]florbetapir (98). The comparison to AC with a gold standard CT was performed both globally and regionally, with a special focus on robustness and outlier analysis. The average performance in PET tracer uptake was within ±5% of CT for all of the proposed methods, with the average±SD global percentage bias in PET FDG uptake for each method being: MR-ACDIXON (-11.3±3.5)%, MR-ACUTE (-5.7±2.0)%, MR-ACONTARIO (-4.3±3.6)%, MR-ACMUNICH (3.7±2.1)%, MR-ACMLAA (-1.9±2.6)%, MR-ACSEGBONE (-1.7±3.6)%, MR-ACUCL (0.8±1.2)%, MR-ACCAR-RiDR (-0.4±1.9)%, MR-ACMAXPROB (-0.4±1.6)%, MR-ACBOSTON (-0.3±1.8)%, and MR-ACRESOLUTE (0.3±1.7)%, ordered by average bias. The overall best performing methods (MR-ACBOSTON, MR-ACMAXPROB, MR-ACRESOLUTE and MR-ACUCL, ordered alphabetically) showed regional average errors within ±3% of PET with CT-AC in all regions of the brain with FDG, and the same four methods, as well as MR-ACCAR-RiDR, showed that for 95% of the patients, 95% of brain voxels had an uptake that deviated by less than 15% from the reference. Comparable performance was obtained with PiB and florbetapir. All of the proposed novel methods have an average global performance within likely acceptable limits (±5% of CT-based reference), and the main difference among the methods was found in the robustness, outlier analysis, and clinical feasibility. Overall, the best performing methods were MR-ACBOSTON, MR-ACMAXPROB, MR-ACRESOLUTE and MR-ACUCL, ordered alphabetically. These methods all minimized the number of outliers, standard deviation, and average global and local error. The methods MR-ACMUNICH and MR-ACCAR-RiDR were both within acceptable quantitative limits, so these methods should be considered if processing time is a factor. The method MR-ACSEGBONE also demonstrates promising results, and performs well within the likely acceptable quantitative limits. For clinical routine scans where processing time can be a key factor, this vendor-provided solution currently outperforms most methods. With the performance of the methods presented here, it may be concluded that the challenge of improving the accuracy of MR-AC in adult brains with normal anatomy has been solved to a quantitatively acceptable degree, which is smaller than the quantification reproducibility in PET imaging.