1,230 research outputs found

    Generalized uncertainty principle and correction value to the black hole entropy

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    Recently, there has been much attention devoted to resolving the quantum corrections to the Bekenstein-Hawking entropy of the black hole. In particular, many researchers have expressed a vested interest in the coefficient of the logarithmic term of the black hole entropy correction term. In this paper, we calculate the correction value of the black hole entropy by utilizing the generalized uncertainty principle and obtain the correction term caused by the generalized uncertainty principle. Because in our calculation we think that the Bekenstein-Hawking area theorem is still valid after considering the generalized uncertainty principle, we derive that the coefficient of the logarithmic term of the black hole entropy correction term is negative. This result is different from the known result at present. Our method is valid not only for single horizon spacetime but also for double horizons spacetime. In the whole process, the physics idea is clear and calculation is simple. It offers a new way for studying the condition that Bekenstein-Hawking area theorem is valid

    Effect of B2O3 and P2O5 on fluorosilicic mica glass-ceramic sintering process

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    To study the effect of B2O3 and P2O5 on fluorosilicic mica glass-ceramic sintering process, six sets of K2O-MgO-SiO2-F glasses were prepared by using B2O3 and P2O5 as sintering aid, respectively. Green bodies of the glass powder were formed by gel casting and sintered at 800, 850, 900, 950, 1000oC for 6 hours, resectively. The sintering and crystallization behavior were studied by thermal shrinkage , X-ray diffraction and SEM. The results showed that the shrinkage rate of the glass with 2wt% B2O3 and P2O5 was highest, while the rate of the glass with 5wt% P2O5 was lowest. An additional crystal other than fluorosilicic mica was precipitated in the glass ceramics generated by sintering of glass powder. The present results confirmed that the glass powder of pure K2O-MgO-SiO2-Fsystem had poor sinterability, while glass powder with minor addition of P2O5 and/or B2O3 showed good sinterability. This result was also verified by SEM

    Surgical excision promotes tumor growth and metastasis by promoting expression of MMP-9 and VEGF in a breast cancer model

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    Surgery is still the main curative therapeutic modality for breast cancer. Although surgery often results in the successful removal of the primary tumor, its process could increase the risk of metastases of residual cancer cells. Understanding of the connection between breast cancer metastasis and surgical wound will lead to the establishment of a proper treatment strategy for postoperative cancer patient. Aim: To study the influence of surgical procedure on the metastasis of primary breast cancer. Methods: We established MDA-MB-435 human breast cancer xenograft model. Levels of Pro-matrix metalloproteinase 9 (Pro-MMP-9) and vascular endothelial growth factor (VEGF) in host serum and tumors were tested at different time points with ELISA and zymography and correlated to tumor growth and postoperative metastasis. Results: Our study demonstrated surgical wound had promoting effect on tumor growth and pulmonary metastasis of human breast cells, if tumor cells remain in bodies. This effect might be related to the postoperative interaction of cancer and host cells, which resulted in expression of Pro-MMP-9. Surgical process could also increase the VEGF expression in tumor tissues. Conclusions: Surgical wound-produced host Pro-MMP-9 and tumor cell VEGF might be important mediators leading to metastasis of residual breast cancer after surgery.Π₯ирургичСскоС Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ Π΄ΠΎ сих ΠΏΠΎΡ€ остаСтся Π³Π»Π°Π²Π½Ρ‹ΠΌ тСрапСвтичСским ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠΌ ΠΏΡ€ΠΈ Π»Π΅Ρ‡Π΅Π½ΠΈΠΈ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… Ρ€Π°ΠΊΠΎΠΌ ΠΌΠΎΠ»ΠΎΡ‡Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ‹. Π₯отя хирургичСскоС ΡƒΠ΄Π°Π»Π΅Π½ΠΈΠ΅ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ Π² Π±ΠΎΠ»ΡŒΡˆΠΈΠ½ΡΡ‚Π²Π΅ случаСв достаточно эффСктивно, Π² Ρ‚ΠΎ ΠΆΠ΅ врСмя ΠΎΠ½ΠΎ ΠΌΠΎΠΆΠ΅Ρ‚ ΡƒΠ²Π΅Π»ΠΈΡ‡ΠΈΡ‚ΡŒ риск мСтастазирования остаточных ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ. ПониманиС связи ΠΌΠ΅ΠΆΠ΄Ρƒ мСтастазированиСм ΠΏΡ€ΠΈ Ρ€Π°ΠΊΠ΅ ΠΌΠΎΠ»ΠΎΡ‡Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ‹ ΠΈ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ Ρ€Π°Π½ΠΎΠΉ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ‚ Π²Ρ‹Π±Ρ€Π°Ρ‚ΡŒ Π½Π°ΠΈΠ»ΡƒΡ‡ΡˆΡƒΡŽ ΡΡ‚Ρ€Π°Ρ‚Π΅Π³ΠΈΡŽ постопСрационного лСчСния. ЦСль: ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΠΈΡ‚ΡŒ влияниС хирургичСского Π²ΠΌΠ΅ΡˆΠ°Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π° Π½Π° мСтастазированиС ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: Π±Ρ‹Π»Π° создана модСль Ρ€Π°ΠΊΠ° ΠΌΠΎΠ»ΠΎΡ‡Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ‹ Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ° Π² Π²ΠΈΠ΄Π΅ ксСнотрансплантата MDA-MB-435. Π£Ρ€ΠΎΠ²Π΅Π½ΡŒ Pro-ΠΌΠ°Ρ‚Ρ€ΠΈΡ‡Π½ΠΎΠΉ ΠΌΠ΅Ρ‚Π°Π»Π»ΠΎΠΏΡ€ΠΎΡ‚Π΅ΠΈΠ½Π°Π·Ρ‹ 9 (Pro-MMP-9) ΠΈ Ρ„Π°ΠΊΡ‚ΠΎΡ€Π° роста эндотСлия сосудов (VEGF) Π² сывороткС Ρ€Π΅Ρ†ΠΈΠΏΠΈΠ΅Π½Ρ‚Π° ΠΈ опухолях ΠΎΡ†Π΅Π½ΠΈΠ²Π°Π»ΠΈΡΡŒ Π² Ρ€Π°Π·Π½Ρ‹Π΅ Π²Ρ€Π΅ΠΌΠ΅Π½Π½Ρ‹Π΅ ΠΏΡ€ΠΎΠΌΠ΅ΠΆΡƒΡ‚ΠΊΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ELISA ΠΈ Π·ΠΈΠΌΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ. ΠŸΡ€ΠΈ этом опрСдСляли Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ корСлляции ΠΌΠ΅ΠΆΠ΄Ρƒ этими ΠΏΠΎΠΊΠ°Π·Π°- ΠΈ Π·ΠΈΠΌΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ. ΠŸΡ€ΠΈ этом опрСдСляли Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ корСлляции ΠΌΠ΅ΠΆΠ΄Ρƒ этими ΠΏΠΎΠΊΠ°Π·Π° ΠΈ Π·ΠΈΠΌΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ. ΠŸΡ€ΠΈ этом опрСдСляли Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ корСлляции ΠΌΠ΅ΠΆΠ΄Ρƒ этими показатСлями, ростом ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ ΠΈ постопСрационными мСтастазами. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: Π±Ρ‹Π»ΠΎ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ опСрационная Ρ€Π°Π½Π° способствуСт росту ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ ΠΌΠΎΠ»ΠΎΡ‡Π½ΠΎΠΉ ΠΆΠ΅Π»Π΅Π·Ρ‹ ΠΈ Π΅Π΅ ΠΌΠ΅Ρ‚Π°ΡΡ‚Π°Π·ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡŽ Π² Π»Π΅Π³ΠΊΠΈΠ΅ Π² случаС, ΠΊΠΎΠ³Π΄Π° ΠΏΡ€ΠΈ ΡƒΠ΄Π°Π»Π΅Π½ΠΈΠΈ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ Π² Ρ€Π°Π½Π΅ ΠΎΡΡ‚Π°ΡŽΡ‚ΡΡ ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹Π΅ ΠΊΠ»Π΅Ρ‚ΠΊΠΈ. Π­Ρ‚ΠΎ ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ связано с постопСрационным взаимодСйствиСм ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹Ρ… ΠΈ ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰ΠΈΡ… ΠΈΡ… Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ, ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ΅ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ экспрСссии Pro-MMP-9. Π£Π΄Π°Π»Π΅Π½ΠΈΠ΅ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ ΠΌΠΎΠΆΠ΅Ρ‚ Ρ‚Π°ΠΊΠΆΠ΅ ΡΠΏΠΎΡΠΎΠ±ΡΡ‚Π²ΠΎΠ²Π°Ρ‚ΡŒ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΡŽ экспрСссии VEGF ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹ΠΌΠΈ ΠΊΠ»Π΅Ρ‚ΠΊΠ°ΠΌΠΈ. Π’Ρ‹Π²ΠΎΠ΄Ρ‹: Pro-MMP-9, экспрСссируСмый Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ ΠΊΠ»Π΅Ρ‚ΠΊΠ°ΠΌΠΈ, ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰ΠΈΠΌΠΈ ΠΏΠΎΡΡ‚ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΡƒΡŽ Ρ€Π°Π½Ρƒ, Π° Ρ‚Π°ΠΊΠΆΠ΅ VEGF, ΠΏΡ€ΠΎΠ΄ΡƒΡ†ΠΈΡ€ΡƒΠ΅ΠΌΡ‹ΠΉ ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹ΠΌΠΈ ΠΊΠ»Π΅Ρ‚ΠΊΠ°ΠΌΠΈ, ΠΌΠΎΠ³ΡƒΡ‚ Π±Ρ‹Ρ‚ΡŒ Π²Π°ΠΆΠ½Ρ‹ΠΌΠΈ ΠΌΠ΅Π΄ΠΈΠ°Ρ‚ΠΎΡ€Π°ΠΌΠΈ мСтастазирования остаточных ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ послС хирургичСского Π²ΠΌΠ΅ΡˆΠ°Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π°

    Isotope effects and possible pairing mechanism in optimally doped cuprate superconductors

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    We have studied the oxygen-isotope effects on T_{c} and in-plane penetration depth \lambda_{ab}(0) in an optimally doped 3-layer cuprate Bi_{1.6}Pb_{0.4}Sr_{2}Ca_{2}Cu_{3}O_{10+y} (T_{c} \sim 107 K). We find a small oxygen-isotope effect on T_{c} (\alpha_{O} = 0.019), and a substantial effect on \lambda_{ab} (0) (\Delta \lambda_{ab} (0)/\lambda_{ab} (0) = 2.5\pm0.5%). The present results along with the previously observed isotope effects in single-layer and double-layer cuprates indicate that the isotope exponent \alpha_{O} in optimally doped cuprates is small while the isotope effect on the in-plane effective supercarrier mass is substantial and nearly independent of the number of the CuO_{2} layers. A plausible pairing mechanism is proposed to explain the isotope effects, high-T_{c} superconductivity and tunneling spectra in a consistent way.Comment: 5 pages, 4 figure

    High-pressure behaviors of carbon nanotubes

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    In this paper, we have reviewed the experimental and theoretical studies on pressure-induced polygonization, ovalization, racetrack–shape deformation, and polymerization of carbon nanotubes (CNTs). The corresponding electronic, optical, and mechanical changes accompanying these behaviors have been discussed. The transformations of armchair (n, n) CNT bundles (n = 2, 3, 4, 6, and 8) under hydrostatic or nonhydrostatic pressure into new carbons, including recently proposed superhard bct-Cβ‚„, Cco-Cβ‚ˆ, and B-B1AL2R2 carbon phases have also been demonstrated. Given the diversity of CNTs from various chiralities, diameters, and arrangements, pressure-induced CNT polymerization provides a promising approach to produce numerous novel metastable carbons exhibiting unique electronic, optical, and mechanical characteristics.Розглянуто Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ– Ρ‚Π° Ρ‚Π΅ΠΎΡ€Π΅Ρ‚ΠΈΡ‡Π½Ρ– дослідТСння Π· Ρ–Π½Π΄ΡƒΠΊΠΎΠ²Π°Π½ΠΎΡŽ тиском ΠΏΠΎΠ»Ρ–Π³ΠΎΠ½Ρ–Π·Π°Ρ†Ρ–Ρ—, ΠΎΠ²Π°Π»Ρ–Π·Π°Ρ†Ρ–Ρ—, Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†Ρ–Ρ— Ρƒ Ρ„ΠΎΡ€ΠΌΡ– Π±Ρ–Π³ΠΎΠ²ΠΎΡ— Π΄ΠΎΡ€Ρ–ΠΆΠΊΠΈ Ρ– ΠΏΠΎΠ»Ρ–ΠΌΠ΅Ρ€ΠΈΠ·Π°Ρ†Ρ–Ρ— Π²ΡƒΠ³Π»Π΅Ρ†Π΅Π²ΠΈΡ… Π½Π°Π½ΠΎΡ‚Ρ€ΡƒΠ±ΠΎΠΊ (ВНВ). ΠžΠ±Π³ΠΎΠ²ΠΎΡ€Π΅Π½ΠΎ Π²Ρ–Π΄ΠΏΠΎΠ²Ρ–Π΄Π½Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½Ρ–, ΠΎΠΏΡ‚ΠΈΡ‡Π½Ρ– Ρ– ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½Ρ– Π·ΠΌΡ–Π½ΠΈ, Ρ‰ΠΎ ΡΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΆΡƒΡŽΡ‚ΡŒ Ρ†Ρ– процСси. Π’Π°ΠΊΠΎΠΆ продСмонстровано пСрСтворСння Π² ВНВ Ρƒ Ρ„ΠΎΡ€ΠΌΡ– крісла (n, n), Π·Ρ–Π±Ρ€Π°Π½ΠΈΡ… Π² ΠΏΡƒΡ‡ΠΎΠΊ (n = 2, 3, 4, 6 Ρ– 8) ΠΏΡ–Π΄ гідростатичним Π°Π±ΠΎ нСгідростатичним тиском Π² Π½ΠΎΠ²Ρ– Π²ΡƒΠ³Π»Π΅Ρ†Π΅Π²Ρ– Π°Π»ΠΎΡ‚Ρ€ΠΎΠΏΠΈ, Π² Ρ‚ΠΎΠΌΡƒ числі Π½Π΅Π΄Π°Π²Π½ΠΎ Π·Π°ΠΏΡ€ΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½Ρ– Π½Π°Π΄Ρ‚Π²Π΅Ρ€Π΄Ρ– bct-Cβ‚„, Cco-Cβ‚ˆ Ρ– B-B1AL2R2-Π²ΡƒΠ³Π»Π΅Ρ†Π΅Π²Ρ– Ρ„Π°Π·ΠΈ. Π Ρ–Π·Π½ΠΎΠΌΠ°Π½Ρ–Ρ‚Π½Ρ–ΡΡ‚ΡŒ ВНВ Π· Ρ€Ρ–Π·Π½ΠΈΠΌΠΈ Ρ…Ρ–Ρ€Π°Π»ΡŒΠ½Ρ–ΡΡ‚ΡŽ, Π΄Ρ–Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ Ρ‚Π° ΡƒΠΏΠ°ΠΊΠΎΠ²ΠΊΠ°ΠΌΠΈ, Π° Ρ‚Π°ΠΊΠΎΠΆ полімСризація ВНВ, Π²ΠΈΠΊΠ»ΠΈΠΊΠ°Π½Π° тиском, Π·Π°Π±Π΅Π·ΠΏΠ΅Ρ‡ΡƒΡ” пСрспСктивний ΠΏΡ–Π΄Ρ…Ρ–Π΄ для отримання числСнних Π½ΠΎΠ²ΠΈΡ… ΠΌΠ΅Ρ‚Π°ΡΡ‚Π°Π±Ρ–Π»ΡŒΠ½ΠΈΡ… Π²ΡƒΠ³Π»Π΅Ρ†Π΅Π²ΠΈΡ… Ρ„Π°Π·, Ρ‰ΠΎ Π΄Π΅ΠΌΠΎΠ½ΡΡ‚Ρ€ΡƒΡŽΡ‚ΡŒ ΡƒΠ½Ρ–ΠΊΠ°Π»ΡŒΠ½Ρ– Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½Ρ–, ΠΎΠΏΡ‚ΠΈΡ‡Π½Ρ– Ρ– ΠΌΠ΅Ρ…Π°Π½Ρ–Ρ‡Π½Ρ– характСристики.РассмотрСны ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ ΠΈ тСорСтичСскиС исслСдования ΠΏΠΎ ΠΈΠ½Π΄ΡƒΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΉ Π΄Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎΠ»ΠΈΠ³ΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ, ΠΎΠ²Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ, Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ Π² Ρ„ΠΎΡ€ΠΌΠ΅ Π±Π΅Π³ΠΎΠ²ΠΎΠΉ Π΄ΠΎΡ€ΠΎΠΆΠΊΠΈ ΠΈ ΠΏΠΎΠ»ΠΈΠΌΠ΅Ρ€ΠΈΠ·Π°Ρ†ΠΈΠΈ ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½Ρ‹Ρ… Π½Π°Π½ΠΎΡ‚Ρ€ΡƒΠ±ΠΎΠΊ (УНВ). ΠžΠ±ΡΡƒΠΆΠ΄Π΅Π½Ρ‹ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠ΅ элСктронныС, оптичСскиС ΠΈ мСханичСскиС измСнСния, ΡΠΎΠΏΡ€ΠΎΠ²ΠΎΠΆΠ΄Π°ΡŽΡ‰ΠΈΠ΅ эти процСссы. Π’Π°ΠΊΠΆΠ΅ продСмонстрированы прСобразования Π² УНВ Π² Ρ„ΠΎΡ€ΠΌΠ΅ крСсла (n, n), собранных Π² ΠΏΡƒΡ‡ΠΎΠΊ (n = 2, 3, 4, 6 ΠΈ 8) ΠΏΠΎΠ΄ гидростатичСским ΠΈΠ»ΠΈ нСгидростатичСским Π΄Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ Π² Π½ΠΎΠ²Ρ‹Π΅ ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½Ρ‹Π΅ Π°Π»Π»ΠΎΡ‚Ρ€ΠΎΠΏΡ‹, Π² Ρ‚ΠΎΠΌ числС Π½Π΅Π΄Π°Π²Π½ΠΎ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½Ρ‹Π΅ свСрхтвСрдыС bct-Cβ‚„, Cco-Cβ‚ˆ ΠΈ B-B1AL2R2-ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½Ρ‹Π΅ Ρ„Π°Π·Ρ‹. Π Π°Π·Π½ΠΎΠΎΠ±Ρ€Π°Π·ΠΈΠ΅ УНВ с Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌΠΈ Ρ…ΠΈΡ€Π°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒΡŽ, Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ ΠΈ ΡƒΠΏΠ°ΠΊΠΎΠ²ΠΊΠ°ΠΌΠΈ, Π° Ρ‚Π°ΠΊΠΆΠ΅ полимСризация УНВ, вызванная Π΄Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ, обСспСчиваСт пСрспСктивный ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ для получСния многочислСнных Π½ΠΎΠ²Ρ‹Ρ… ΠΌΠ΅Ρ‚Π°ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½Ρ‹Ρ… ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½Ρ‹Ρ… Ρ„Π°Π·, Π΄Π΅ΠΌΠΎΠ½ΡΡ‚Ρ€ΠΈΡ€ΡƒΡŽΡ‰ΠΈΡ… ΡƒΠ½ΠΈΠΊΠ°Π»ΡŒΠ½Ρ‹Π΅ элСктронныС, оптичСскиС ΠΈ мСханичСскиС характСристики

    Large extraordinary Hall effect in [Pt/Co]5/Ru/[Co/Pt]5 multilayer

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    This Brief Report presents giant extraordinary Hall effect (EHE) in the Ru-mediated antiferromagnetically coupled [Pt/Co]5/Ru/[Co/Pt]5 multilayers (MLs) compared with those MLs without the Ru spacer. The enhancement of the EHE is attributed to the strong Ru/Co interface scattering. Through the variation in the Pt layer thickness and the temperature, we determine the relation between the Hall voltage and the longitudinal resistivity. It is found that the conventional scaling analysis has difficulties in consistently interpreting our data

    Boty-II, a novel LTR retrotransposon in Botrytis cinerea B05.10 revealed by genomic sequence

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    Botrytis cinerea is a necrotrophic pathogen causing pre- and post-harvest diseases in at least 235 plant species. It manifests extraordinary genotype and phenotype variation. One of the causes of this variation is transposable elements. Two transposable elements have been discovered in this fungus, the retrotransposon (Boty), and the transposon (Flipper). In this work, two complete (Boty-II-76 and Boty-II-103) and two partial (Boty-II-95 and Boty-II-141) long terminal repeat (LTR) retrotransposons were identified by an in silico genomic sequence analysis. Boty-II-76 and Boty-II-103 contain 6439 bp nucleotides with a pair of LTRs at both ends, and an internal deduced pol gene encoding a polyprotein with reverse transcriptase and DDE integrase domains. They are flanked by 5 bp direct repeats (ACCAT, CTTTC). In Boty-II-141, two LTRs at both ends, and a partial internal pol gene encoding a protein with a DDE integrase domain were identified. In Boty-II-95, a right LTR and a partial internal pol gene encoding a protein with no conserved domains were identified. Boty-II uses a self-priming mechanism to initiate synthesis of reverse transcripts. The sequence of the presumed primer binding site for first-strand reverse transcription is 5'-TTGTACCAT-3'. The polypurine-rich sequence for plus-strand DNA synthesis is 5'-GCCTTGAGCGGGGGGTAC-3'. Fourteen Boty-II LTRs that contain 125-158 bp nucleotides and share 69.1 ~ 100% identities with the short inverted terminal repeats of 5 bp (TGTCA\u2026TGACA) were discovered. Analysis of structural features and phylogeny revealed that Boty-II is a novel LTR retrotransposon. It could potentially be used as a novel molecular marker for the investigation of genetic variation in B. cinerea

    Ultrastrong conductive in situ composite composed of nanodiamond incoherently embedded in disordered multilayer graphene

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    Traditional ceramics or metals cannot simultaneously achieve ultrahigh strength and high electrical conductivity. The elemental carbon can form a variety of allotropes with entirely different physical properties, providing versatility for tuning mechanical and electrical properties in a wide range. Here, by precisely controlling the extent of transformation of amorphous carbon into diamond within a narrow temperature–pressure range, we synthesize an in situ composite consisting of ultrafine nanodiamond homogeneously dispersed in disordered multilayer graphene with incoherent interfaces, which demonstrates a Knoop hardness of up to ~53 GPa, a compressive strength of up to ~54 GPa and an electrical conductivity of 670–1,240 S m(–1) at room temperature. With atomically resolving interface structures and molecular dynamics simulations, we reveal that amorphous carbon transforms into diamond through a nucleation process via a local rearrangement of carbon atoms and diffusion-driven growth, different from the transformation of graphite into diamond. The complex bonding between the diamond-like and graphite-like components greatly improves the mechanical properties of the composite. This superhard, ultrastrong, conductive elemental carbon composite has comprehensive properties that are superior to those of the known conductive ceramics and C/C composites. The intermediate hybridization state at the interfaces also provides insights into the amorphous-to-crystalline phase transition of carbon

    Identifying topological edge states in 2D optical lattices using light scattering

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    We recently proposed in a Letter [Physical Review Letters 108 255303] a novel scheme to detect topological edge states in an optical lattice, based on a generalization of Bragg spectroscopy. The scope of the present article is to provide a more detailed and pedagogical description of the system - the Hofstadter optical lattice - and probing method. We first show the existence of topological edge states, in an ultra-cold gas trapped in a 2D optical lattice and subjected to a synthetic magnetic field. The remarkable robustness of the edge states is verified for a variety of external confining potentials. Then, we describe a specific laser probe, made from two lasers in Laguerre-Gaussian modes, which captures unambiguous signatures of these edge states. In particular, the resulting Bragg spectra provide the dispersion relation of the edge states, establishing their chiral nature. In order to make the Bragg signal experimentally detectable, we introduce a "shelving method", which simultaneously transfers angular momentum and changes the internal atomic state. This scheme allows to directly visualize the selected edge states on a dark background, offering an instructive view on topological insulating phases, not accessible in solid-state experiments.Comment: 17 pages, 10 figures. Revised and extended version, to appear in EJP Special Topic for the special issue on "Novel Quantum Phases and Mesoscopic Physics in Quantum Gases". Extended version of arXiv:1203.124
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