422 research outputs found
Visualization of longitudinally-oriented intermediate filaments in frozen sections of chicken cardiac muscle by a new staining method.
Magnetic skyrmion lattices in heavy fermion superconductor UPt3
Topological analysis of nearly SO(3)_{spin} symmetric Ginzburg--Landau
theory, proposed for UPt by Machida et al, shows that there exists a new
class of solutions carrying two units of magnetic flux: the magnetic skyrmion.
These solutions do not have singular core like Abrikosov vortices and at low
magnetic fields they become lighter for strongly type II superconductors.
Magnetic skyrmions repel each other as at distances much larger then the
magnetic penetration depth , forming a relatively robust triangular
lattice. The magnetic induction near is found to increase as
. This behavior agrees well with experiments.Comment: 4 pages, 2 figures, 2 column format; v2:misprint in the title is
correcte
Passage of an integral membrane protein, the vesicular stomatitis virus glycoprotein, through the Golgi apparatus en route to the plasma membrane.
Magnetic skyrmions and their lattices in triplet superconductors
Complete topological classification of solutions in SO(3) symmetric
Ginzburg-Landau free energy has been performed and a new class of solutions in
weak external magnetic field carrying two units of magnetic flux has been
identified. These solutions, magnetic skyrmions, do not have singular core like
Abrikosov vortices and at low magnetic field become lighter for strongly type
II superconductors. As a consequence, the lower critical magnetic field Hc1 is
reduced by a factor of log(kappa). Magnetic skyrmions repel each other as 1/r
at distances much larger then magnetic penetration depth forming relatively
robust triangular lattice. Magnetic induction near Hc1 increases gradually as
(H-Hc1)^2. This agrees very well with experiments on heavy fermion
superconductor UPt3. Newly discovered Ru based compounds Sr2RuO4 and
Sr2YRu(1-x)Cu(x)O6 are other possible candidates to possess skyrmion lattices.
Deviations from exact SO(3) symmetry are also studied.Comment: 23 pages, 10 eps figure
Microtubules in Bacteria: Ancient Tubulins Build a Five-Protofilament Homolog of the Eukaryotic Cytoskeleton
Microtubules play crucial roles in cytokinesis, transport, and motility, and are therefore superb targets for anti-cancer drugs. All tubulins evolved from a common ancestor they share with the distantly related bacterial cell division protein FtsZ, but while eukaryotic tubulins evolved into highly conserved microtubule-forming heterodimers, bacterial FtsZ presumably continued to function as single homopolymeric protofilaments as it does today. Microtubules have not previously been found in bacteria, and we lack insight into their evolution from the tubulin/FtsZ ancestor. Using electron cryomicroscopy, here we show that the tubulin homologs BtubA and BtubB form microtubules in bacteria and suggest these be referred to as “bacterial microtubules” (bMTs). bMTs share important features with their eukaryotic counterparts, such as straight protofilaments and similar protofilament interactions. bMTs are composed of only five protofilaments, however, instead of the 13 typical in eukaryotes. These and other results suggest that rather than being derived from modern eukaryotic tubulin, BtubA and BtubB arose from early tubulin intermediates that formed small microtubules. Since we show that bacterial microtubules can be produced in abundance in vitro without chaperones, they should be useful tools for tubulin research and drug screening
Sub-Dominant Pairing Channels in Unconventional Superconductors: Ginzburg-Landau Theory
A Ginzburg-Landau theory is developed for unconventional superconductors with
the three relevant singlet pairing channels. Various consequences of the
sub-dominant channels (i.e., s- and d_{xy}-channels) are examined in detail.
(1) In the case of a d_{x^2-y^2}+is-wave superconductor, The structure of a
single vortex above and below T_{DS} is four-fold and two-fold symmetric,
respectively. (2) In the case of a d_{x^2-y^2}+id_{xy}-wave superconductor,
there is also a second order zero-field phase transition from the pure
d_{x^2-y^2}-phase to the Time-reversal-symmetry-breaking
d_{x^2-y^2}+id_{xy}-wave phase at the temperature T_{DD'}. But the subdominant
phase can (not) be induced by vortices above T_{DD'}. Below the time-reversal-
symmetry-breaking transition, the sub-dominant phase in the mixed state is
nontrivial: it survives at low fields, but may disappear above a field
(increasing with decreasing temperature) presumably via a first-order
transition. (3)By including the strong coupling effects, a
time-reversal-symmetry -breaking coupling term between the d_{x^2-y^2}- and
d_{xy}-waves is found to have significant effects on the low temperature
behavior of d_{x^2-y^2}+id_{xy} superconductors. In a magnetic field, a
d_{x^2-y^2}+id_{xy} state is always established, but the field-dependence of
d_{xy}-amplitude above T_{DD'} is different from that below T_{DD'}. Above but
not very close to T_{DD'}, the induced minimum gap Delta_0 proportional to
B/(T-T_{DD'}).Comment: updated, 7 two-column pages with one embedded figure, one formula
corrected, to appear in Phys. Rev. B 6
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