64 research outputs found
Endovascular treatments for ischemic stroke: Present status and prospects
Endovascular treatments for ischemic stroke (IS) are coming into clinical practice and, as shown by recent investigations, have good prospects. These treatments for IS make it possible to expand indications for revascularization and to create prerequisite for improving the outcomes of treatment.Interventional treatments for IS should not be set off against intravenous thrombolytic therapy (ITT); it is necessary to seek their reasonable sharing. The promising directions in the development of ITT and endovascular revascularization (EVR) for IS are to upgrade tools and to choose the safest and most effective constructions, as well as to identify target patient groups needing these treatment options based on the prediction of the efficacy of these techniques with consideration for clinical findings, the pattern of a lesion, and radiological data (including estimates of perfusion, ischemic core-penumbra relationships, and collateral blood supply intensity).The paper discusses the present status and prospects of EVR of cerebrovascular arteries, its indications, and basic procedures
ΠΠΠΠ―ΠΠΠ ΠΠΠ£ΠΠΠΠΠ ΠΠΠΠ‘Π’ΠΠΠΠ ΠΠ ΠΠΠΠΠΠΠΠΠΠΠΠΠ ΠΠΠ‘ΠΠΠΠΠΠ ΠΠ¦ΠΠΠΠΠΠ ΠΠΠΠΠΠ’ΠΠΠΠΠ ΠΠΠ‘Π€Π£ΠΠΠ¦ΠΠ
The profound deepening of medicamentous sleep down to the burst-suppression electroencephalography pattern is used to provide medication-based protection of brain during preventive temporary clipping of the major arteries when performing surgery due to cerebral aneurysms. There is no consensus about the effect of profound suppression of electrobiological activity on the development of post-operative cognitive dysfunction. The goal: to evaluate the impact of anesthesia with the burst-suppression electroencephalography pattern on the post-operative cognitive status of the patients with no cerebral disorders. Subjects and methods. 30 patients were enrolled into the prospective randomized study, they all had surgeries due to degenerative spinal diseases. All patients were divided into two groups. Anesthesia in the main group (Group 1) differed from the one in the control group (Group 2); it included administration of propofol till achieving suppression of the electrobiological activity of burst-suppression electroencephalography pattern during 15 minutes. Prior to the surgery and in 4 days after it, all patients had neuro-psychological tests using Montreal Cognitive Assessment (MoCA), Frontal Assessment Battery (FAB) and numbers memorization techniques (NMT). Results. When testing in 4 days after surgery, results in the patients from Group 1 did not differ from pre-operative results of MoCA (Mebefore =Β 28, Meafter= 28, Z = 0.714, p = 0.476), FAB (Mebefore = 18, Meafter = 18, Z = 0.592, p = 0.554), memorization of numbers in the direct order (Mebefore = 18, Meafter = 18, Z = 0.178, p = 0.859) and in the reverse order (Mebefore = 18, Meafter = 18, Z = 0.548, p = 0.583). The results of the post-operative testing in Group 2 were compatible with pre-operative results of (Mebefore = 18, Meafter = 18, Z = 0.459, p = 0.646), FAB (Mebefore = 18, Meafter = 18, Z =Β 1.348, p =Β 0.178), memorization of numbers in the direct order (Mebefore = 18, Meafter = 18, Z = 0.21, p = 0.843) and in the reverse order (Mebefore =Β 18, Meafter =Β 18, Z = 0.809, p = 0.418). None of the tests detected significant differences between the Groups (U = 88, p = 0.319, Z = 0.995 for MoCA; UΒ =Β 102.5, p = 0.644, Z = 0.394 for FAB; U = 92.0, p = 0.407, Z = -0.829 for memorization of numbers in the direct order, and U = 33.5, p = 0.62, ZΒ =Β 0.572 for memorization of numbers in the reverse order). Conclusion. Anesthesia with burst-suppression electroencephalography pattern as a model of medication-based cerebral protection during temporary clipping of the major arteries does not cause the deterioration of cognitive status in the patients who had no cerebral pathology initially.Β ΠΠ»Ρ ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½ΡΠΎΠ·Π½ΠΎΠΉ Π·Π°ΡΠΈΡΡ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° Π² ΠΏΠ΅ΡΠΈΠΎΠ΄ ΠΏΡΠ΅Π²Π΅Π½ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΊΠ»ΠΈΠΏΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ°Π³ΠΈΡΡΡΠ°Π»ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ ΠΏΡΠΈ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΡΡ
ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρ ΡΠ΅ΡΠ΅Π±ΡΠ°Π»ΡΠ½ΡΡ
Π°Π½Π΅Π²ΡΠΈΠ·ΠΌ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΡΠ³Π»ΡΠ±Π»Π΅Π½ΠΈΠ΅ ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½ΡΠΎΠ·Π½ΠΎΠ³ΠΎ ΡΠ½Π° Π΄ΠΎ ΠΏΠΎΡΠ²Π»Π΅Π½ΠΈΡ Π½Π° ΡΠ»Π΅ΠΊΡΡΠΎΡΠ½ΡΠ΅ΡΠ°Π»ΠΎΠ³ΡΠ°ΠΌΠΌΠ΅ ΠΏΠ°ΡΡΠ΅ΡΠ½Π° Β«Π²ΡΠΏΡΡΠΊΠ° β ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅Β». ΠΠ΅Ρ Π΅Π΄ΠΈΠ½ΠΎΠ³ΠΎ ΠΌΠ½Π΅Π½ΠΈΡ Π² ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠΈ Π²Π»ΠΈΡΠ½ΠΈΡ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΠ³Π½Π΅ΡΠ΅Π½ΠΈΡ Π±ΠΈΠΎΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π½Π° Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠ΅ ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΠΊΠΎΠ³Π½ΠΈΡΠΈΠ²Π½ΠΎΠΉ Π΄ΠΈΡΡΡΠ½ΠΊΡΠΈΠΈ. Π¦Π΅Π»Ρ: ΠΎΡΠ΅Π½ΠΈΡΡ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π°Π½Π΅ΡΡΠ΅Π·ΠΈΠΈ Ρ ΡΠ»Π΅ΠΊΡΡΠΎΡΠ½ΡΠ΅ΡΠ°Π»ΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΠ°ΡΡΠ΅ΡΠ½ΠΎΠΌ Β«Π²ΡΠΏΡΡΠΊΠ° β ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅Β» Π½Π° ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΡΠΉ ΠΊΠΎΠ³Π½ΠΈΡΠΈΠ²Π½ΡΠΉ ΡΡΠ°ΡΡΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π±Π΅Π· ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°. ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π ΠΏΡΠΎΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠΌ ΡΠ°Π½Π΄ΠΎΠΌΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΡΡΠ°ΡΡΠ²ΠΎΠ²Π°Π»ΠΈ 30 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠΌ Π²ΡΠΏΠΎΠ»Π½ΠΈΠ»ΠΈ Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π»Π΅ΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρ Π΄Π΅Π³Π΅Π½Π΅ΡΠ°ΡΠΈΠ²Π½ΡΡ
Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ ΠΏΠΎΠ·Π²ΠΎΠ½ΠΎΡΠ½ΠΈΠΊΠ°. ΠΡΠ΅ ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ Π±ΡΠ»ΠΈ ΡΠ°Π·Π΄Π΅Π»Π΅Π½Ρ Π½Π° Π΄Π²Π΅ Π³ΡΡΠΏΠΏΡ. ΠΠ½Π΅ΡΡΠ΅Π·ΠΈΡ Π² ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ (1-Ρ Π³ΡΡΠΏΠΏΠ°) ΠΎΡΠ»ΠΈΡΠ°Π»Π°ΡΡ ΠΎΡ ΠΊΠΎΠ½ΡΡΠΎΠ»ΡΠ½ΠΎΠΉ (2-Ρ Π³ΡΡΠΏΠΏΠ°) Π²Π²Π΅Π΄Π΅Π½ΠΈΠ΅ΠΌ ΠΏΡΠΎΠΏΠΎΡΠΎΠ»Π° Π΄ΠΎ ΠΏΠΎΡΠ²Π»Π΅Π½ΠΈΡ Π² Π±ΠΈΠΎΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° ΠΏΠ°ΡΡΠ΅ΡΠ½Π° Β«Π²ΡΠΏΡΡΠΊΠ° β ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅Β» Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 15 ΠΌΠΈΠ½. ΠΠ΅ΡΠ΅Π΄ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ΅ΠΉ ΠΈ Π½Π° 4-Π΅ ΡΡΡ ΠΏΠΎΡΠ»Π΅ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° Π²ΡΠ΅ΠΌ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π΅ΠΉΡΠΎΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ΅ΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΠΎΠ½ΡΠ΅Π°Π»ΡΡΠΊΠΎΠΉ ΡΠΊΠ°Π»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ ΠΏΡΠΈΡ
ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ½ΠΊΡΠΈΠΉ (MoCA), Π±Π°ΡΠ°ΡΠ΅ΠΈ ΡΠ΅ΡΡΠΎΠ² Π΄Π»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ Π»ΠΎΠ±Π½ΠΎΠΉ Π΄ΠΈΡΡΡΠ½ΠΊΡΠΈΠΈ (FAB) ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ Π·Π°ΠΏΠΎΠΌΠΈΠ½Π°Π½ΠΈΡ ΡΠΈΡΡ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΡΠΈ ΠΎΠ±ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ Π½Π° 4-Π΅ ΡΡΡ ΠΏΠΎΡΠ»Π΅ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ Π² 1-ΠΉ Π³ΡΡΠΏΠΏΠ΅ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π½Π΅ ΠΎΡΠ»ΠΈΡΠ°Π»ΠΈΡΡ ΠΎΡ ΠΏΡΠ΅Π΄ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠ΅ΡΡΠΎΠ² MoCA (MeΠ΄ΠΎ = 28, MeΠΏΠΎΡΠ»Π΅ = 28, Z = 0,714, p = 0,476), FAB (MeΠ΄ΠΎ = 18, MeΠΏΠΎΡΠ»Π΅ = 18, Z = 0,592, p = 0,554), Π·Π°ΠΏΠΎΠΌΠΈΠ½Π°Π½ΠΈΡ ΡΠΈΡΡ Π² ΠΏΡΡΠΌΠΎΠΌ (MeΠ΄ΠΎ = 18, MeΠΏΠΎΡΠ»Π΅ = 18, Z = 0,178, p = 0,859) ΠΈ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ (MeΠ΄ΠΎ = 18, MeΠΏΠΎΡΠ»Π΅ = 18, Z = 0,548, p = 0,583). ΠΠΎ 2-ΠΉ Π³ΡΡΠΏΠΏΠ΅ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΎΠ±ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π±ΡΠ»ΠΈ ΡΠΎΠΏΠΎΡΡΠ°Π²ΠΈΠΌΡ Ρ ΠΏΡΠ΅Π΄ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΡΠΌΠΈ Π΄Π°Π½Π½ΡΠΌΠΈ ΡΠ΅ΡΡΠΎΠ² MoCA (MeΠ΄ΠΎ = 18, MeΠΏΠΎΡΠ»Π΅ = 18, ZΒ =Β 0,459, p = 0,646), FAB (MeΠ΄ΠΎ = 18, MeΠΏΠΎΡΠ»Π΅ = 18, Z = 1,348, p = 0,178), Π·Π°ΠΏΠΎΠΌΠΈΠ½Π°Π½ΠΈΡ ΡΠΈΡΡ Π² ΠΏΡΡΠΌΠΎΠΌ (MeΠ΄ΠΎ = 18, MeΠΏΠΎΡΠ»Π΅ = 18, Z = 0,21, p = 0,843) ΠΈ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ (MeΠ΄ΠΎ = 18, MeΠΏΠΎΡΠ»Π΅ = 18, Z = 0,809, p = 0,418). ΠΠ΅ΠΆΠ΄Ρ 1-ΠΉ ΠΈ 2-ΠΉ Π³ΡΡΠΏΠΏΠ°ΠΌΠΈ Π·Π½Π°ΡΠΈΠΌΡΡ
ΠΎΡΠ»ΠΈΡΠΈΠΉ Π½Π΅ Π²ΡΡΠ²Π»Π΅Π½ΠΎ Π½ΠΈ ΠΏΠΎ ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊ (U = 88, p = 0,319, Z = 0,995 Π΄Π»Ρ MoCA; U = 102,5, p = 0,644, Z = 0,394 Π΄Π»Ρ FAB; U = 92,0, p = 0,407, Z = -0,829 Π΄Π»Ρ Π·Π°ΠΏΠΎΠΌΠΈΠ½Π°Π½ΠΈΡ Π² ΠΏΡΡΠΌΠΎΠΌ ΠΈ U = 33,5, p = 0,62, Z = 0,572 Π΄Π»Ρ Π·Π°ΠΏΠΎΠΌΠΈΠ½Π°Π½ΠΈΡ Π² ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅). ΠΡΠ²ΠΎΠ΄. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π°Π½Π΅ΡΡΠ΅Π·ΠΈΠΈ Ρ ΡΠ»Π΅ΠΊΡΡΠΎΡΠ½ΡΠ΅ΡΠ°Π»ΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΠ°ΡΡΠ΅ΡΠ½ΠΎΠΌ Β«Π²ΡΠΏΡΡΠΊΠ° β ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅Β» ΠΊΠ°ΠΊ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½ΡΠΎΠ·Π½ΠΎΠΉ Π·Π°ΡΠΈΡΡ ΠΌΠΎΠ·Π³Π° Π½Π° ΠΏΠ΅ΡΠΈΠΎΠ΄ Π²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΊΠ»ΠΈΠΏΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ°Π³ΠΈΡΡΡΠ°Π»ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ Π½Π΅ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΡ
ΡΠ΄ΡΠ΅Π½ΠΈΡ ΠΊΠΎΠ³Π½ΠΈΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΡΡΠ°ΡΡΡΠ° ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π±Π΅Π· ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°.
High-field magnetic structure of the triangular antiferromagnet RbFe(MoO4)2
The magnetic H β T phase diagram of a quasi-two-dimensional antiferromagnet RbFe(MoO4 )2 (S = 5/2) with an equilateral triangular lattice structure is studied with 87Rb NMR and neutron-diffraction techniques. This combination of experimental techniques allows us to determine the ordered components of the magnetic moments on the Fe3+ ions within various high-field phasesβthe Y, UUD, V, and fan structures, stabilized in the compound by the in-plane magnetic field. It is also established that the transition from the V to the fan phase is of first order, whereas the transition from the fan phase to the polarized paramagnetic phase is continuous. An analysis of the NMR spectra shows that the high-field fan phase of RbFe(MoO4 )2 can be successfully described by a periodic commensurate oscillation of the magnetic moments around the field direction in each Fe3+ layer combined with an incommensurate modulation of the magnetic structure perpendicular to the layers
New high magnetic field phase of the frustrated chain compound LiCuVO
Magnetization of the frustrated chain compound LiCuVO, focusing
on high magnetic field phases, is reported. Besides a spin-flop transition and
the transition from a planar spiral to a spin modulated structure observed
recently, an additional transition was observed just below the saturation
field. This newly observed magnetic phase is considered as a spin nematic
phase, which was predicted theoretically but was not observed experimentally.
The critical fields of this phase and its dM/dH curve are in good agreement
with calculations performed in a microscopic model (M. E. Zhitomirsky and H.
Tsunetsugu, preprint, arXiv:1003.4096v2).Comment: 5 pages, 4 figure
Magnetic properties and revisited exchange integrals of the frustrated chain cuprate PbCuSO(OH) - linarite
We present a detailed study in the paramagnetic regime of the frustrated
= 1/2 spin-compound linarite, PbCuSO(OH), with competing ferromagnetic
nearest-neighbor and antiferromagnetic next-nearest-neighbor exchange
interactions. Our data reveal highly anisotropic values for the saturation
field along the crystallographic main directions, with 7.6, 10.5
and 8.5\,T for the , , and axes, respectively. In the
paramagnetic regime, this behavior is explained mainly by the anisotropy of the
\textit{g}-factor but leaving room for an easy-axis exchange anisotropy. Within
the isotropic - spin model our experimental data are described by
various theoretical approaches yielding values for the exchange interactions
-100\,K and 36\,K. These main intrachain exchange
integrals are significantly larger as compared to the values derived in two
previous studies in the literature and shift the frustration ratio 0.36 of linarite closer to the 1D critical point at 0.25.
Electron spin resonance (ESR) and nuclear magnetic resonance (NMR) measurements
further prove that the static susceptibility is dominated by the intrinsic spin
susceptibility. The Knight shift as well as the broadening of the linewidth in
ESR and NMR at elevated temperatures indicate a highly frustrated system with
the onset of magnetic correlations far above the magnetic ordering temperature
= 2.75(5)\,K, in agreement with the calculated exchange
constants.Comment: 18 pages, 18 figure
Π Π΅ΡΡΠ°ΠΊΡΠ΅ΡΠ½ΡΠΉ ΡΠΏΠΈΠ»Π΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΡΠ°ΡΡΡ ΠΏΠΎΡΠ»Π΅ ΠΊΠ»ΠΈΠΏΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π°Π½Π΅Π²ΡΠΈΠ·ΠΌΡ ΡΡΠ΅Π΄Π½Π΅ΠΉ ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ (ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΠ΅)
We present the management features for the refractory epileptic status in a patient after surgical treatment of unruptured cerebral aneurysm and no epileptic prehistory. The role of continuous electroencephalographic monitoring in adjusting the rate of drugs administration for general anesthesia in the treatment of this condition is also described.ΠΡΠΈΠ²Π΅Π΄Π΅Π½Π° Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠ°ΡΠΈΡ ΠΈ ΠΎΠ±ΡΡΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠ΅ΠΉ Π²Π΅Π΄Π΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΊΠΈ Ρ ΡΠ΅ΡΡΠ°ΠΊΡΠ΅ΡΠ½ΡΠΌ ΡΠΏΠΈΠ»Π΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΡΠ°ΡΡΡΠΎΠΌ ΠΏΠΎΡΠ»Π΅ Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ Π½Π΅ΡΠ°Π·ΠΎΡΠ²Π°Π²ΡΠ΅ΠΉΡΡ Π°Π½Π΅Π²ΡΠΈΠ·ΠΌΡ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° Π±Π΅Π· ΡΠΏΠΈΠ»Π΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π½Π°ΠΌΠ½Π΅Π·Π°. ΠΠΎΠΊΠ°Π·Π°Π½Π° ΡΠΎΠ»Ρ Π½Π΅ΠΏΡΠ΅ΡΡΠ²Π½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΊΡΡΠΎΡΠ½ΡΠ΅ΡΠ°Π»ΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΠ½Π³Π° Π΄Π»Ρ ΠΏΠΎΠ΄Π±ΠΎΡΠ° ΡΠΊΠΎΡΠΎΡΡΠΈ Π²Π²Π΅Π΄Π΅Π½ΠΈΡ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² Π΄Π»Ρ ΠΎΠ±ΡΠ΅ΠΉ Π°Π½Π΅ΡΡΠ΅Π·ΠΈΠΈ ΠΏΡΠΈ Π»Π΅ΡΠ΅Π½ΠΈΠΈ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ
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