2,567 research outputs found
Dynamics of myelin content decrease in the rat stroke model
The majority of studies were usually focused on neuronal death after brain ischemia; however, stroke affects all cell types including oligodendrocytes that form myelin sheath in the CNS. Our study is focused on the changes of myelin content in the ischemic core and neighbor structures in early terms (1, 3 and 10 days) after stroke. Stroke was modeled with middle cerebral artery occlusion (MCAo) in 15 male rats that were divided into three groups by time points after operation. Brain sections were histologically stained with Luxol Fast Blue (LFB) for myelin quantification. The significant demyelination was found in the ischemic core, corpus callosum, anterior commissure, whereas myelin content was increased in caudoputamen, internal capsule and piriform cortex compared with the contralateral hemisphere. The motor cortex showed a significant increase of myelin content on the 1st day and a significant decrease on the 3rd and 10th days after MCAo. These results suggest that stroke influences myelination not only in the ischemic core but also in distant structures
Passive mode locking of a Tm,Ho:KY(WO4)(2) laser around 2 ΞΌm
We report the first demonstration, to our knowledge, of passive mode locking in a Tm3+, Ho3+-codoped KYWO42 laser operating in the 2000-2060 nm spectral region. An InGaAsSb-based quantum well semiconductor saturable absorber mirror is used for the initiation and stabilization of the ultrashort pulse generation. Pulses as short as 3.3 ps were generated at 2057 nm with average output powers up to 315 mW at a pulse repetition frequency of 132 MHz for 1.15 W of absorbed pump power at 802 nm from a Ti:sapphire laser
Π§Π°ΡΡΠΈΡΠ° ΡΠΎ ΡΠΏΠΈΠ½ΠΎΠΌ 1/2 Ρ Π°Π½ΠΎΠΌΠ°Π»ΡΠ½ΡΠΌ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠΌ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ Π΄ΠΈΠΏΠΎΠ»ΡΠ½ΡΠΌ ΠΌΠΎΠΌΠ΅Π½ΡΠ°ΠΌΠΈ
It is Petras who first developed the P-symmetric theory for a spin 1/2 particle with an anomalous magnetic moment within the general Gelβfand β Yaglom approach. Recently, similarly it was introduced a P-asymmetric wave equation for a spin 1/2 particle which describes a particle with an electric dipole moment. In this paper, we study solutions of the equation for the P-asymmetric particle in presence of external magnetic fields. It turns out that the energy spectra are the same for P-asymmetric and P-symmetric particles. To clarify this coincidence, we demonstrate that there exists a simple transformation relating these two models, by which one wave equation can be reduced to the form of the other. Meanwhile, expressions for wave functions and P-reflection operators are different in these two theories. We extend this approach to the model in which both P-symmetric and P-asymmetric sectors are presented. The main result is the same, namely, there exists a simple, more general as compared with the mentioned above transformation relating the P-symmetric model and the model with two sectors, and expressions for wave functions and P-reflection operators are different in these two bases. We demonstrate that in the presence of an external uniform magnetic field, the energy spectra in the model with two sectors coincide with those in the P-symmetric theory. Thus, we develop a general theory for the P-asymmetric model and the model with two sectors within the Petras approach.P-ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½Π°Ρ ΡΠ΅ΠΎΡΠΈΡ ΡΠ°ΡΡΠΈΡΡ Ρ Π°Π½ΠΎΠΌΠ°Π»ΡΠ½ΡΠΌ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠΌ ΠΌΠΎΠΌΠ΅Π½ΡΠΎΠΌ Π±ΡΠ»Π° ΡΠ°Π·Π²ΠΈΡΠ° ΠΠ΅ΡΡΠ°ΡΠ΅ΠΌ Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΠΎΠ±ΡΠ΅Π³ΠΎ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Π° ΠΠ΅Π»ΡΡΠ°Π½Π΄Π° β Π―Π³Π»ΠΎΠΌΠ°. ΠΠ΅Π΄Π°Π²Π½ΠΎ Π² ΡΠ°ΠΌΠΊΠ°Ρ
Π°Π½Π°Π»ΠΎΠ³ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Π° Π±ΡΠ»ΠΎ Π²Π²Π΅Π΄Π΅Π½ΠΎ P-Π°ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΠΎΠ΅ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΅ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ Π΄Π»Ρ ΡΠ°ΡΡΠΈΡΡ ΡΠΎ ΡΠΏΠΈΠ½ΠΎΠΌ 1/2, ΠΊΠΎΡΠΎΡΠΎΠ΅ ΠΎΠΏΠΈΡΡΠ²Π°Π΅Ρ ΡΠ°ΡΡΠΈΡΡ Ρ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ Π΄ΠΈΠΏΠΎΠ»ΡΠ½ΡΠΌ ΠΌΠΎΠΌΠ΅Π½ΡΠΎΠΌ. Π Π½Π°ΡΡΠΎΡΡΠ΅ΠΉ ΡΠ°Π±ΠΎΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΡΡΡΡΡ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Π΄Π»Ρ P-Π°ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΠΎΠΉ ΡΠ°ΡΡΠΈΡΡ Π² ΠΏΡΠΈΡΡΡΡΡΠ²ΠΈΠΈ Π²Π½Π΅ΡΠ½ΠΈΡ
ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΏΠΎΠ»Π΅ΠΉ. ΠΠΊΠ°Π·Π°Π»ΠΎΡΡ, ΡΡΠΎ ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠΏΠ΅ΠΊΡΡ P-Π°ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΠΎΠΉ ΡΠ°ΡΡΠΈΡΡ ΡΠ°ΠΊΠΎΠΉ ΠΆΠ΅, ΠΊΠ°ΠΊ Ρ P-ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΠΎΠΉ ΡΠ°ΡΡΠΈΡΡ. ΠΠ»Ρ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΡ ΡΡΠΎΠ³ΠΎ ΡΠΎΠ²ΠΏΠ°Π΄Π΅Π½ΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΡΡΠ΅ΡΡΠ²ΡΠ΅Ρ ΠΏΡΠΎΡΡΠΎΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅, Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΠΎΠ΄Π½ΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΅ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΏΡΠΈΠ²Π΅Π΄Π΅Π½ΠΎ ΠΊ Π²ΠΈΠ΄Ρ Π΄ΡΡΠ³ΠΎΠ³ΠΎ, ΠΏΡΠΈ ΡΡΠΎΠΌ Π²ΡΡΠ°ΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ Π²ΠΎΠ»Π½ΠΎΠ²ΡΡ
ΡΡΠ½ΠΊΡΠΈΠΉ ΠΈ ΠΎΠΏΠ΅ΡΠ°ΡΠΎΡΠΎΠ² P-ΠΎΡΡΠ°ΠΆΠ΅Π½ΠΈΡ ΡΠ°Π·Π»ΠΈΡΠ½Ρ Π² ΡΡΠΈΡ
Π΄Π²ΡΡ
ΡΠ΅ΠΎΡΠΈΡΡ
. ΠΠ°Π½Π½ΡΠΉ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ ΠΎΠ±ΠΎΠ±ΡΠ΅Π½ Π½Π° ΠΌΠΎΠ΄Π΅Π»Ρ, Π² ΠΊΠΎΡΠΎΡΠΎΠΉ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΠΎΠ±Π° ΡΠ΅ΠΊΡΠΎΡΠ°: P-ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΡΠΉ ΠΈ P-Π°ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΡΠΉ. ΠΡΠ½ΠΎΠ²Π½ΠΎΠΉ ΡΠ΅Π·ΡΠ»ΡΡΠ°Ρ ΠΎΠΊΠ°Π·Π°Π»ΡΡ ΡΠ΅ΠΌ ΠΆΠ΅: ΡΡΡΠ΅ΡΡΠ²ΡΠ΅Ρ ΠΏΡΠΎΡΡΠΎΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅, Π±ΠΎΠ»Π΅Π΅ ΠΎΠ±ΡΠ΅Π΅, ΡΠ΅ΠΌ ΡΠΊΠ°Π·Π°Π½Π½ΠΎΠ΅ Π²ΡΡΠ΅, ΡΠ²ΡΠ·ΡΠ²Π°ΡΡΠ΅Π΅ P-ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΡΡ ΠΌΠΎΠ΄Π΅Π»Ρ ΠΈ ΠΌΠΎΠ΄Π΅Π»Ρ Ρ Π΄Π²ΡΠΌΡ ΡΠ΅ΠΊΡΠΎΡΠ°ΠΌΠΈ, Π²ΡΡΠ°ΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ Π²ΠΎΠ»Π½ΠΎΠ²ΡΡ
ΡΡΠ½ΠΊΡΠΈΠΉ ΠΈ ΠΎΠΏΠ΅ΡΠ°ΡΠΎΡΠΎΠ² P-ΠΎΡΡΠ°ΠΆΠ΅Π½ΠΈΡ ΡΠ°Π·Π»ΠΈΡΠ½Ρ Π² ΡΡΠΈΡ
Π΄Π²ΡΡ
Π±Π°Π·ΠΈΡΠ°Ρ
. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΡΠΈ Π½Π°Π»ΠΈΡΠΈΠΈ Π²Π½Π΅ΡΠ½Π΅Π³ΠΎ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠΏΠ΅ΠΊΡΡΡ Π² ΠΌΠΎΠ΄Π΅Π»ΠΈ Ρ Π΄Π²ΡΠΌΡ ΡΠ΅ΠΊΡΠΎΡΠ°ΠΌΠΈ ΡΠΎΠ²ΠΏΠ°Π΄Π°ΡΡ Ρ ΡΠ°ΠΊΠΎΠ²ΡΠΌΠΈ Π² P-ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΠΎΠΉ ΡΠ΅ΠΎΡΠΈΠΈ. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ, ΡΠ°Π·Π²ΠΈΡΠ° ΠΎΠ±ΡΠ°Ρ ΡΠ΅ΠΎΡΠΈΡ P-Π°ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈ ΠΌΠΎΠ΄Π΅Π»ΠΈ Ρ Π΄Π²ΡΠΌΡ ΡΠ΅ΠΊΡΠΎΡΠ°ΠΌΠΈ Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Π° ΠΠ΅ΡΡΠ°ΡΠ°
Increased Sensitivity to Possible Muonium to Antimuonium Conversion
A new experimental search for muonium-antimuonium conversion was conducted at
the Paul Scherrer Institute, Villigen, Switzerland. The preliminary analysis
yielded one event fulfilling all required criteria at an expected background of
1.7(2) events due to accidental coincidences. An upper limit for the conversion
probability in 0.1 T magnetic field is extracted as (90%
CL).Comment: 2 figure
Spin 1/2 particle with anomalous magnetic and electric dipole moments theories with one and three mass parameters
In this paper, we study solutions of the equation for the P-asymmetric particle with spin Β½ in presence of external magnetic fields. It turns out that energy spectra are the same for P-asymmetric and P-symmetric particles
Π§Π°ΡΡΠΈΡΠ° ΡΠΎ ΡΠΏΠΈΠ½ΠΎΠΌ 1/2 Ρ Π°Π½ΠΎΠΌΠ°Π»ΡΠ½ΡΠΌ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠΌ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ Π΄ΠΈΠΏΠΎΠ»ΡΠ½ΡΠΌ ΠΌΠΎΠΌΠ΅Π½ΡΠ°ΠΌΠΈ
It is Petras who first developed the P-symmetric theory for a spin 1/2 particle with an anomalous magnetic
moment within the general Gelβfand β Yaglom approach. Recently, similarly it was introduced a P-asymmetric wave equation
for a spin 1/2 particle which describes a particle with an electric dipole moment. In this paper, we study solutions of the
equation for the P-asymmetric particle in presence of external magnetic fields. It turns out that the energy spectra are the
same for P-asymmetric and P-symmetric particles. To clarify this coincidence, we demonstrate that there exists a simple
transformation relating these two models, by which one wave equation can be reduced to the form of the other. Meanwhile,
expressions for wave functions and P-reflection operators are different in these two theories. We extend this approach to
the model in which both P-symmetric and P-asymmetric sectors are presented. The main result is the same, namely, there
exists a simple, more general as compared with the mentioned above transformation relating the P-symmetric model and
the model with two sectors, and expressions for wave functions and P-reflection operators are different in these two bases.
We demonstrate that in the presence of an external uniform magnetic field, the energy spectra in the model with two sectors
coincide with those in the P-symmetric theory. Thus, we develop a general theory for the P-asymmetric model and the model
with two sectors within the Petras approach
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