Charles H. Mielke

Dr. Charles H. Mielke

Los Alamos National Lab, Los Alamos, NM, USA
orcid

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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24 August 2001 in Journal of Physics: Condensed Matter
Verified
Journal Article
Closed access
PDF file
CMCharles H. Mielke
Charles H. Mielke
JSJohn Singleton
John Singleton
MNMoon-Sun Nam
Moon-Sun Nam
NHNeil Harrison
Neil Harrison
CAC C Agosta
C C Agosta
LML K Montgomery
L K Montgomery

1 September 2006 in Journal of Physics and Chemistry of Solids
Verified
Journal Article
Closed access
RMRoss D. McDonald
Ross D. McDonald
PGPaul A. Goddard
Paul A. Goddard
JLJason Lashley
Jason Lashley
NHNeil Harrison
Neil Harrison
CMCharles H. Mielke
Charles H. Mielke
MSMichi-To Suzuki
Michi-To Suzuki

1 August 2001 in arXiv
Verified
Preprint
Open access
PDF file
CMCharles H. Mielke
Charles H. Mielke
JSJohn Singleton
John Singleton
MNMoon-Sun Nam
Moon-Sun Nam
NHNeil Harrison
Neil Harrison
CAC. C. Agosta
C. C. Agosta
LML. K. Montgomery
L. K. Montgomery
The Fermi surface topology of the organic superconductor \lbets has been determined using the Shubnikov-de Haas and magnetic breakdown effects and angle-dependent magnetoresistance oscillations. The former experiments were carried out in pulsed fields of up to 60 T, whereas the latter employed quasistatic fields of up to 30 T. All of these data show that the Fermi-surface topology of \lbets is very similar to that of the most heavily-studied organic superconductor, \cuscn, except in one important respect; the interplane transfer integral in \lbets is a factor $\sim 10$ larger than that in \cuscn . The increased three-dimensionality of \lbets is manifested in radiofrequency penetration-depth measurements, which show a clear dimensional crossover in the behaviour of $H_{c2}(T)$. The radiofrequency measurements have also been used to extract the Labusch parameter determining the fluxoid interactions as a function of temperature, and to map the flux-lattice melting curve.