2,974 research outputs found
Recurrent aggressive chondrosarcoma of the middle phalanx of the index finger: excision and reconstruction with an osteocartilaginous allograft
Introduction: Chondrosarcomas are malignant tumours and need to be treated aggressively including ablative surgery. BovΓ©e et al. and Mankin have recently drawn attention to a less aggressive behaviour of chondrosarcomas of the phalanges compared with those of other localizations including the metacarpals. Materials and methods: An 12year follow-up of a patient with a chondrosarcoma of the middle phalanx of the index finger is presented. The lesion was curetted initially, and a repeat curettage was performed 4years later. Finally, 8years later the phalanx was excised and reconstructed with an osteocartilaginous allograft. Histologically, the lesion changed from a chondrosarcoma grade I to grade II. Result: The patient continues to be free of recurrence and metastases 4years after the final resection. Conclusion: The potential for systemic disease of chondrosarcomas of the phalanges is probably much lower than in chondrosarcomas of other localizations, and therefore digit-sparing techniques may be considered rather than ablative procedure
Coulomb blockade and transport in a chain of one-dimensional quantum dots
A long one-dimensional wire with a finite density of strong random impurities
is modelled as a chain of weakly coupled quantum dots. At low temperature T and
applied voltage V its resistance is limited by "breaks": randomly occuring
clusters of quantum dots with a special length distribution pattern that
inhibits the transport. Due to the interplay of interaction and disorder
effects the resistance can exhibit T and V dependences that can be approximated
by power laws. The corresponding two exponents differ greatly from each other
and depend not only on the intrinsic electronic parameters but also on the
impurity distribution statistics.Comment: 4 pages, 1 figure. Changes from v2: Dropped discussion of the
high-field regime. Added discussion of mesoscopic fluctuations and multiple
channels in the quasi-1D case. Improved presentation styl
Two-dimensional electron gas formation in undoped In[0.75]Ga[0.25]As/In[0.75]Al[0.25]As quantum wells
We report on the achievement of a two-dimensional electron gas in completely
undoped In[0.75]Al[0.25]As/In[0.75]Ga[0.25]As metamorphic quantum wells. Using
these structures we were able to reduce the carrier density, with respect to
reported values in similar modulation-doped structures. We found experimentally
that the electronic charge in the quantum well is likely due to a deep-level
donor state in the In[0.75]Al[0.25]As barrier band gap, whose energy lies
within the In[0.75]Ga[0.25]As/In[0.75]Al[0.25]As conduction band discontinuity.
This result is further confirmed through a Poisson-Schroedinger simulation of
the two-dimensional electron gas structure.Comment: 17 pages, 6 figures, to be published in J. Vac. Sci. Technol.
The AMS-RICH velocity and charge reconstruction
The AMS detector, to be installed on the International Space Station,
includes a Ring Imaging Cerenkov detector with two different radiators, silica
aerogel (n=1.05) and sodium fluoride (n=1.334). This detector is designed to
provide very precise measurements of velocity and electric charge in a wide
range of cosmic nuclei energies and atomic numbers. The detector geometry, in
particular the presence of a reflector for acceptance purposes, leads to
complex Cerenkov patterns detected in a pixelized photomultiplier matrix. The
results of different reconstruction methods applied to test beam data as well
as to simulated samples are presented. To ensure nominal performances
throughout the flight, several detector parameters have to be carefully
monitored. The algorithms developed to fulfill these requirements are
presented. The velocity and charge measurements provided by the RICH detector
endow the AMS spectrometer with precise particle identification capabilities in
a wide energy range. The expected performances on light isotope separation are
discussed.Comment: Contribution to the ICRC07, Merida, Mexico (2007); Presenter: F.
Bara
Quantum creep and variable range hopping of one-dimensional interacting electrons
The variable range hopping results for noninteracting electrons of Mott and
Shklovskii are generalized to 1D disordered charge density waves and Luttinger
liquids using an instanton approach. Following a recent paper by Nattermann,
Giamarchi and Le Doussal [Phys. Rev. Lett. {\bf 91}, 56603 (2003)] we calculate
the quantum creep of charges at zero temperature and the linear conductivity at
finite temperatures for these systems. The hopping conductivity for the short
range interacting electrons acquires the same form as for noninteracting
particles if the one-particle density of states is replaced by the
compressibility. In the present paper we extend the calculation to dissipative
systems and give a discussion of the physics after the particles materialize
behind the tunneling barrier. It turns out that dissipation is crucial for
tunneling to happen. Contrary to pure systems the new metastable state does not
propagate through the system but is restricted to a region of the size of the
tunneling region. This corresponds to the hopping of an integer number of
charges over a finite distance. A global current results only if tunneling
events fill the whole sample. We argue that rare events of extra low tunneling
probability are not relevant for realistic systems of finite length. Finally we
show that an additional Coulomb interaction only leads to small logarithmic
corrections.Comment: 15 pages, 3 figures; references adde
Dynamic Fluctuation Phenomena in Double Membrane Films
Dynamics of double membrane films is investigated in the long-wavelength
limit including the overdamped squeezing mode. We demonstrate that thermal
fluctuations essentially modify the character of the mode due to its nonlinear
coupling to the transversal shear hydrodynamic mode. The corresponding Green
function acquires as a function of the frequency a cut along the imaginary
semi-axis. Fluctuations lead to increasing the attenuation of the squeezing
mode it becomes larger than the `bare' value.Comment: 7 pages, Revte
The RICH detector of the AMS-02 experiment: status and physics prospects
The Alpha Magnetic Spectrometer (AMS), whose final version AMS-02 is to be
installed on the International Space Station (ISS) for at least 3 years, is a
detector designed to measure charged cosmic ray spectra with energies up to the
TeV region and with high energy photon detection capability up to a few hundred
GeV. It is equipped with several subsystems, one of which is a proximity
focusing RICH detector with a dual radiator (aerogel+NaF) that provides
reliable measurements for particle velocity and charge. The assembly and
testing of the AMS RICH is currently being finished and the full AMS detector
is expected to be ready by the end of 2008. The RICH detector of AMS-02 is
presented. Physics prospects are briefly discussed.Comment: 5 pages. Contribution to the 10th ICATPP Conference on Astroparticle,
Particle, Space Physics, Detectors and Medical Physics Applications (Como
2007). Presenter: Rui Pereir
ΠΠΊΡΡΡΠ°ΡΠ°ΡΡΠΈΠ°Π»ΡΠ½Π°Ρ Π³Π΅ΠΌΠΈΡΠΈΡΠ΅ΠΎΠΈΠ΄ΡΠΊΡΠΎΠΌΠΈΡ
The aim of the study was to improve surgical results of patients having thyroid gland pathology by the development of the surgery method directed to increasing possibility of injury and maintenance of the upper laryngeal nerve integrity. Method of performing extrafascial hemithyreoidectomy with visualization of recurrent nerve, parathyroid gland and upper thyroid artery is presented which is directed to decrease specific complications (vocal fold paresis, hypoparathyreosis) and complications associated with the upper laryngeal nerve injury. Using this method, 166 patients having node pathology of thyroid gland were operated on. This method resulted in decreased number of complications (from 15,0 to 2,6%).Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ - ΡΠ»ΡΡΡΠ΅Π½ΠΈΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠ΅ΠΉ ΡΠΈΡΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ ΠΏΡΡΠ΅ΠΌ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π°, Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½Π½ΠΎΠΉ Π½Π° ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ Π²Π΅ΡΠΎΡΡΠ½ΠΎΡΡΠΈ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ ΠΈ ΡΠΎΡ
ΡΠ°Π½Π΅Π½ΠΈΠ΅ ΡΠ΅Π»ΠΎΡΡΠ½ΠΎΡΡΠΈ Π²Π΅ΡΡ
Π½Π΅Π³ΠΎ Π³ΠΎΡΡΠ°Π½Π½ΠΎΠ³ΠΎ Π½Π΅ΡΠ²Π°. ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π° ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΡΠΊΡΡΡΠ°ΡΠ°ΡΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π³Π΅ΠΌΠΈΡΠΈΡΠ΅ΠΎΠΈΠ΄ΡΠΊΡΠΎΠΌΠΈΠΈ Ρ Π²ΠΈΠ·ΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ Π²ΠΎΠ·Π²ΡΠ°ΡΠ½ΠΎΠ³ΠΎ Π½Π΅ΡΠ²Π°, ΠΏΠ°ΡΠ°ΡΠΈΡΠΎΠ²ΠΈΠ΄Π½ΡΡ
ΠΆΠ΅Π»Π΅Π· ΠΈ Π²Π΅ΡΡ
Π½Π΅ΠΉ ΡΠΈΡΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ, ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΡΡΡΠ°Ρ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ - ΠΏΠ°ΡΠ΅Π·Π° Π³ΠΎΠ»ΠΎΡΠΎΠ²ΡΡ
ΡΠΊΠ»Π°Π΄ΠΎΠΊ, Π³ΠΈΠΏΠΎΠΏΠ°ΡΠ°ΡΠΈΡΠ΅ΠΎΠ·Π° ΠΈ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ, ΡΠ²ΡΠ·Π°Π½Π½ΡΡ
Ρ ΡΡΠ°Π²ΠΌΠΎΠΉ Π²Π΅ΡΡ
Π½Π΅Π³ΠΎ Π³ΠΎΡΡΠ°Π½Π½ΠΎΠ³ΠΎ Π½Π΅ΡΠ²Π°. ΠΠΎ Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ΅ ΠΏΡΠΎΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½ΠΎ 116 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΡΠ·Π»ΠΎΠ²ΠΎΠΉ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠ΅ΠΉ ΡΠΈΡΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ. ΠΠ»Π°Π³ΠΎΠ΄Π°ΡΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ ΡΠ΄Π°Π»ΠΎΡΡ ΡΠ½ΠΈΠ·ΠΈΡΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ Ρ 15,0 Π΄ΠΎ 2,6%
ΠΡΠ΄Π°Π»Π΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΡΠ·Π»ΠΎΠ²ΠΎΠ³ΠΎ Π·ΠΎΠ±Π°
Long-term results of surgical treatment of 649 patients with different morphological forms of nodular goiter in terms of 15 to 3 years are analyzed. Postsurgical recurrent goiter was diagnosed in 26.8% (174 people). The most part of relapses falls on operations characterized by the large part of TG tissue rest (resection of TG lobe and node enucleation): 69.1% (139 patients of 201). No one relapse was diagnosed after thyreoidectomy. After extremely subtotal resection, relapses were observed in 2.2% (7 people of 312) and after hemithyroidectomy in 20.6% (26 people of 136). This study indicates inadequacy of operations such as node enucleation and resection of the lobe with a node, especially, if the node belongs to nodular colloid goiter, because in such operations the pathologically changed TG tissue is often rest and there is high probability of relapse.ΠΡΠΎΡΠ»Π΅ΠΆΠ΅Π½Ρ ΠΎΡΠ΄Π°Π»Π΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ 649 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΠΌΠΎΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠΎΡΠΌΠ°ΠΌΠΈ ΡΠ·Π»ΠΎΠ²ΠΎΠ³ΠΎ Π·ΠΎΠ±Π° Π² ΡΡΠΎΠΊΠΈ ΠΎΡ 3 Π΄ΠΎ 15 Π»Π΅Ρ. ΠΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΡΠΉ ΡΠ΅ΡΠΈΠ΄ΠΈΠ² ΡΠ·Π»ΠΎΠ²ΠΎΠ³ΠΎ Π·ΠΎΠ±Π° Π±ΡΠ» Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΡΠΎΠ²Π°Π½ Ρ 174 (26,8%) Π±ΠΎΠ»ΡΠ½ΡΡ
. ΠΠΎΠ»ΡΡΠ°Ρ ΡΠ°ΡΡΡ ΡΠ΅ΡΠΈΠ΄ΠΈΠ²ΠΎΠ² ΠΏΡΠΈΡ
ΠΎΠ΄ΠΈΡΡΡ Π½Π° ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΡΠ΅ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π°, Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΡΡΠΈΠ΅ΡΡ ΠΎΡΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ Π±ΠΎΠ»ΡΡΠ΅ΠΉ ΡΠ°ΡΡΠΈ ΡΠΊΠ°Π½ΠΈ ΡΠΈΡΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ, - ΡΠ΅Π·Π΅ΠΊΡΠΈΠΈ Π΄ΠΎΠ»ΠΈ ΠΈ ΡΠ½ΡΠΊΠ»Π΅Π°ΡΠΈΠΈ ΡΠ·Π»ΠΎΠ² - 69,1% (139 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΈΠ· 201). ΠΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΠΎΠ΅ ΡΠΈΡΠ»ΠΎ ΡΠ΅ΡΠΈΠ΄ΠΈΠ²ΠΎΠ² Π²ΠΎΠ·Π½ΠΈΠΊΠ»ΠΎ ΠΏΠΎΡΠ»Π΅ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ, Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΡΡΠΈΡ
ΡΡ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΡΠΌ ΡΠ΄Π°Π»Π΅Π½ΠΈΠ΅ΠΌ ΡΠΊΠ°Π½ΠΈ ΡΠΈΡΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ: ΠΏΡΠ΅Π΄Π΅Π»ΡΠ½ΠΎ-ΡΡΠ±ΡΠΎΡΠ°Π»ΡΠ½ΡΡ ΡΠ΅Π·Π΅ΠΊΡΠΈΡ - 2,2%, ΡΠΈΡΠ΅ΠΎΠΈΠ΄ΡΠΊΡΠΎΠΌΠΈΡ - 0%. ΠΠ°Π½Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠΊΠ°Π·ΡΠ²Π°Π΅Ρ Π½Π° Π½Π΅Π°Π΄Π΅ΠΊΠ²Π°ΡΠ½ΠΎΡΡΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΡΠ°ΠΊΠΈΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ, ΠΊΠ°ΠΊ ΡΠ½ΡΠΊΠ»Π΅Π°ΡΠΈΡ ΡΠ·Π»Π° ΠΈ ΡΠ΅Π·Π΅ΠΊΡΠΈΡ Π΄ΠΎΠ»ΠΈ Ρ ΡΠ·Π»ΠΎΠΌ, ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎ ΠΏΡΠΈ ΠΏΡΠΈΠ½Π°Π΄Π»Π΅ΠΆΠ½ΠΎΡΡΠΈ ΡΠ·Π»Π° ΠΊ ΡΠ·Π»ΠΎΠ²ΠΎΠΌΡ ΠΊΠΎΠ»Π»ΠΎΠΈΠ΄Π½ΠΎΠΌΡ Π·ΠΎΠ±Ρ, ΠΏΠΎΡΠΊΠΎΠ»ΡΠΊΡ ΡΠΎΠΏΡΡΠΆΠ΅Π½Π° Ρ ΠΎΡΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½Π½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ ΠΆΠ΅Π»Π΅Π·Ρ ΠΈ Π±ΠΎΠ»ΡΡΠΎΠΉ Π²Π΅ΡΠΎΡΡΠ½ΠΎΡΡΡΡ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ ΡΠ΅ΡΠΈΠ΄ΠΈΠ²Π° Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΡ
- β¦