1,694 research outputs found

    Disruption of a Yeast ADE6 Gene Homolog in Ustilago maydis

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    A putative homolog of the Sacharromyces cereviseae ADE6 and Escherichia coli purL genes is identified near a multigenic complex, which contains two genes, sid1 and sid2, involved in a siderophore biosynthetic pathway inUstilago maydis. The putative ADE6 homolog was mutated by targeted gene disruption. The resulting mutant strains demonstrated a requirement for exogenous adenine, indicating that the U. maydis ade6 homolog is required for purine biosynthesis

    Clinical impact of MDR1-expression in testicular germ cell cancer

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    Aim: The multidrug resistance protein 1 (MDR1, P-gp, p-170) is a membrane glycoprotein that acts as an energy-dependent drug efflux pump. In various malignancies its expression is associated with resistance to diverse cytostatic drugs, and therefore predicts resistance to systemic treatment. The aim of this study was to investigate the prognostic value of MDR1 expression in primary tumor tissue to predict necrosis or viable cancer in residual tumor masses after systemic chemotherapy for advanced testicular germ cell cancer. Materials and Methods: Out of 77 patients, histopathological characteristics of primary testicular cancer specimens and retroperitoneal lymph node dissection (RPLND) samples following chemotherapy were available from 72 and all 77 patients, respectively. Moreover, MDR1 expression was determined by immunohistochemistry in 47 primary tumors and corresponding 73 RPLND sections. Results: After chemotherapy and subsequent RPLND, the examination of residual tumor masses revealed that mature teratoma and active viable tumor were predominantly found in patients with non-seminoma (NSGCT; p = 0.048), especially in those with containing mature teratoma (p = 0.001). Moreover, using univariate analysis the expression of MDR1 in the primary testicular tumor predicted viable tumor/teratoma residues in RPLND sections (p = 0.003). However, in multivariate analysis including the tumors’ histological subtype, MDR1 expression alone failed to reach statistical significance as an independent prognostic marker for residual vital tumor (p β‰₯ 0.16). Conclusions: With the limited number of patients given, the correlation between MDR1 expression in primary testis cancer and active residual retroperitoneal disease after chemotherapy failed to reach statistical significance as in independent marker. Therefore, up to now routine MDR1 staining of testicular germ cell cancer samples should not be performed in clinical practice. However, as there was a clear trend, a larger number of patients suffering from metastatic non-seminomas should be studied, as MDR1 expression might have significant prognostic value in this particular subgroup of patients.Π‘Π΅Π»ΠΎΠΊ 1 мноТСствСнной лСкарств Π΅Π½Π½ΠΎΠΉ устойчив ости (MDR1, P-gp, p-170) – это ΠΌΠ΅ΠΌΠ±Ρ€Π°Π½Π½Ρ‹ΠΉ Π³Π»ΠΈΠΊΠΎΠΏΡ€ΠΎΡ‚Π΅ΠΈΠ½, Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΉ ΠΊΠ°ΠΊ энСргозависимый насос. ΠŸΡ€ΠΈ Ρ€Π°Π·Π» ΠΈΡ‡Π½Ρ‹Ρ… Ρ„ΠΎ Ρ€ΠΌΠ°Ρ… ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅ΠΉ Π΅Π³ΠΎ экспр Π΅ ссия связана с устойчив ΠΎ ΡΡ‚ΡŒΡŽ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ ΠΊ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌ цитостатикам, Ρ‡Ρ‚ΠΎ ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ использовано для Π²Ρ‹Π±ΠΎΡ€Π° Ρ‚ΠΈΠΏΠ° Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ. ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹ β€” исслСдованиС прогности- чСской значимости экспрСссии MDR1 Π² Ρ‚ΠΊΠ°Π½ΠΈ ΠΏΠ΅ Ρ€Π²ΠΈΡ‡Π½ΠΎΠΉ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ для ΠΎΡ†Π΅Π½ΠΊΠΈ Π²ΠΎΠ·ΠΌΠΎ Тности Ρ€Π°Π· вития Π½Π΅ΠΊΡ€ΠΎΠ·Π° ΠΈΠ»ΠΈ сохран Π΅ ния ΠΆΠΈΠ²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ Π² остаточной Ρ‚ΠΊΠ°Π½ΠΈ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ послС примСнСния систСмной Ρ…ΠΈΠΌΠΈΠΎΡ‚Π΅Ρ€Π°ΠΏΠΈΠΈ Π½Π° ΠΏΠΎΠ·Π΄Π½ΠΈΡ… стадиях Π³Π΅Ρ€ΠΌΠΈΠ½Π°Ρ‚ΠΈΠ²Π½Ρ‹Ρ… ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅ΠΉ яичка. ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹: ΠΏΡ€ΠΎ Π°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎ Π²Π°Π½Ρ‹ гисто ΠΏΠ°Ρ‚ΠΎΠ»ΠΎ гичСскиС Ρ…Π°Ρ€Π°ΠΊΡ‚ Π΅ ристики ΠΏΠ΅ Ρ€Π²ΠΈΡ‡Π½ΠΎ ΠΉ Ρ‚Π΅ стикулярной ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ ΠΈ ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ², ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… ΠΏΡ€ΠΈ иссСчСнии Ρ€Π΅Ρ‚Ρ€ΠΎΠΏΠ΅Ρ€ΠΈΡ‚ΠΎΠ½Π΅Π°Π»ΡŒΠ½Ρ‹Ρ… лимфатичСских ΡƒΠ·Π»ΠΎΠ² (RPLND) послС Ρ…ΠΈΠΌΠΈ ΠΎΡ‚Π΅Ρ€Π°ΠΏΠΈΠΈ 72 ΠΈ 77 Π±ΠΎΠ» ΡŒΠ½Ρ‹Ρ… соотвС тствСнно. Экспр Сссию MDR1 опрСдСляли ΠΈΠΌΠΌΡƒΠ½ огист ΠΎΡ…ΠΈΠΌΠΈΡ‡ Сским ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π² 47 ΠΎΠ±Ρ€Π°Π·Ρ†Π°Ρ… ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½ ΠΎΠΉ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ ΠΈ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… 73 ср RPLND. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: послС Ρ…ΠΈΠΌΠΈ ΠΎΡ‚Π΅Ρ€Π°ΠΏΠΈΠΈ ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΉ RPLNDисслСдовани Π΅ оста- Ρ‚ΠΎΡ‡Π½Ρ‹Ρ… ΠΎΠΏΡƒΡ…ΠΎΠ»Π΅Π²Ρ‹Ρ… Ρ‚ΠΊΠ°Π½Π΅ΠΉ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ, чтозрСлая Ρ‚Π΅Ρ€Π°Ρ‚ΠΎΠΌΠ° ΠΈ ТизнСспособныС ΠΎΠΏΡƒΡ… ΠΎΠ»Π΅Π²Ρ‹Π΅ ΠΊΠ»Π΅Ρ‚ΠΊΠΈ выяв Π»ΡΡŽΡ‚ прСимущСствСнно Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ…, Ρƒ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π½Π΅ Π±Ρ‹Π»Π° ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½Π° сСминома (NSGCT; p = 0,048), особСнно Ρƒ Ρ‚Π°ΠΊ ΠΎΠ²Ρ‹Ρ… , Ρƒ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π±Ρ‹Π»Π° Ρ‚Π΅Ρ€Π°Ρ‚ΠΎΠΌΠ° (p = 0,001). Π‘ΠΎΠ»Π΅Π΅ Ρ‚ΠΎΠ³ΠΎ, Π΄ Π°Π½Π½Ρ‹Π΅ ΠΎΠ΄Π½ΠΎ Ρ„Π°ΠΊΡ‚ΠΎΡ€Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‡Ρ‚ΠΎ экспр Π΅ ссия MDR1 Π² Ρ‚ΠΊΠ°Π½ΠΈ ΠΏΠ΅ Ρ€Π²ΠΈΡ‡Π½ΠΎ ΠΉ Ρ‚Π΅ стику лярной ΠΎΠΏΡƒ- Ρ…ΠΎΠ»ΠΈ ΠΌΠΎΠΆΠ΅Ρ‚ ΡΠ»ΡƒΠΆΠΈΡ‚ΡŒ прогностич Сским Ρ„Π°ΠΊΡ‚ ΠΎΡ€ΠΎΠΌ сохран Сния ΠΆΠΈΠ²Ρ‹Ρ… ΠΎΠΏΡƒΡ… ΠΎΠ»Π΅Π²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ срСзах RPLND (p = 0,003). О Π½Π°ΠΊ ΠΎ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΌΡƒΠ»ΡŒΡ‚ΠΈΡ„Π°ΠΊΡ‚ΠΎΡ€Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°, Π² Ρ‚ΠΎΠΌ числС с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ гистологичСского ΠΏΠΎΠ΄Ρ‚ΠΈΠΏΠ° ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ, ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ, Ρ‡Ρ‚ΠΎ экспр Π΅ ссия MDR1 Π½Π΅ ΠΈΠΌΠ΅Π΅Ρ‚ ΡΠ°ΠΌΠΎΡΡ‚ΠΎΡΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ прогностичСской значимости для выявлСния ΠΆΠΈΠ²Ρ‹Ρ… остаточных ΠΎΠΏΡƒΡ… ΠΎΠ»Π΅Π²Ρ‹Ρ… ΠΊΠ»Π΅Ρ‚ΠΎΠΊ (p 0,16). Π’Ρ‹Π²ΠΎΠ΄Ρ‹: Π²Π²ΠΈΠ΄Ρƒ нСбольшо ΠΉΠ²Ρ‹Π±ΠΎΡ€ΠΊΠΈΠ±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… Π½Π΅ выяв Π»Π΅Π½ΠΎ статистичСски значимойкоррСляции ΠΌΠ΅ΠΆΠ΄Ρƒ экспр СссиСй MDR1 Π² ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½ΠΎΠΉ ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ яичка ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ΠΌ Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… Ρ€Π΅Π·ΠΈΠ΄ΡƒΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΎΡ‡Π°Π³ΠΎΠ² пораТСния Π² Ρ€Π΅Ρ‚Ρ€ΠΎΠΏΠ΅Ρ€ΠΈΡ‚ΠΎΠ½Π΅Π°Π»ΡŒΠ½ΠΎΠΌ пространствС. Π’ Ρ‚ ΠΎ ΠΆΠ΅ врСмя, учитывая Π²Ρ‹ΡΠ²Π»Π΅Π½Π½ΡƒΡŽ Ρ‚Π΅Π½Π΄Π΅Π½Ρ†ΠΈΡŽ, ΡΠΊΡΠΏΡ€Π΅ΡΡΠΈΡŽ MDR1, Π² качСствС Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΠ³ΠΎ прогностич Сского ΠΌΠ°Ρ€ΠΊ Π΅Ρ€Π°, ΠΈΠΌΠ΅Π΅Ρ‚ смысл ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚ΡŒ ΠΈΠΌΠ΅Π½Π½ΠΎ Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… с мСтастатичСскими опухолями, Π½Π΅ ΡΠ²Π»ΡΡŽΡ‰ΠΈΠΌΠΈΡΡ сСминомой

    3-D Interacting CFTs and Generalized Higgs Phenomenon in Higher Spin Theories on AdS

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    We study a duality, recently conjectured by Klebanov and Polyakov, between higher-spin theories on AdS_4 and O(N) vector models in 3-d. These theories are free in the UV and interacting in the IR. At the UV fixed point, the O(N) model has an infinite number of higher-spin conserved currents. In the IR, these currents are no longer conserved for spin s>2. In this paper, we show that the dual interpretation of this fact is that all fields of spin s>2 in AdS_4 become massive by a Higgs mechanism, that leaves the spin-2 field massless. We identify the Higgs field and show how it relates to the RG flow connecting the two CFTs, which is induced by a double trace deformation.Comment: 8 pages, latex; v2 references adde

    Measurement of the electron electric dipole moment using GdIG

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    A new method for the detection of the electron edm using a solid is described. The method involves the measurement of a voltage induced across the solid by the alignment of the samples magnetic dipoles in an applied magnetic field, H. A first application of the method to GdIG has resulted in a limit on the electron edm of 5E-24 e-cm, which is a factor of 40 below the limit obtained from the only previous solid-state edm experiment. The result is limited by the imperfect discrimination of an unexpectedly large voltage that is even upon the reversal of the sample magnetization.Comment: 10 pages, 5 figures, v2:references corrected, submitted to PRL, v3:added labels to figure

    Self-similar solution of a nonsteady problem of nonisothermal vapour condensation on a droplet growing in diffusion regime

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    This paper presents a mathematically exact self-similar solution to the joint nonsteady problems of vapour diffusion towards a droplet growing in a vapour-gas medium and of removal of heat released by a droplet into a vapour-gas medium during vapour condensation. An equation for the temperature of the droplet is obtained; and it is only at that temperature that the self-similar solution exists. This equation requires the constancy of the droplet temperature and even defines it unambiguously throughout the whole period of the droplet growth. In the case of strong display of heat effects, when the droplet growth rate decreases significantly, the equation for the temperature of the droplet is solved analytically. It is shown that the obtained temperature fully coincides with the one that settles in the droplet simultaneously with the settlement of its diffusion regime of growth. At the obtained temperature of the droplet the interrelated nonsteady vapour concentration and temperature profiles of the vapour-gas medium around the droplet are expressed in terms of initial (prior to the nucleation of the droplet) parameters of the vapour-gas medium. The same parameters are used to formulate the law in accordance with which the droplet is growing in diffusion regime, and also to define the time that passes after the nucleation of the droplet till the settlement of diffusion regime of droplet growth, when the squared radius of the droplet becomes proportionate to time. For the sake of completeness the case of weak display of heat effects is been studied.Comment: 12 pages, 4 figure

    Dynamic SU(2) Structure from Seven-branes

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    We obtain a family of supersymmetric solutions of type IIB supergravity with dynamic SU(2) structure, which describe the local geometry near a stack of four D7-branes and one O7-plane wrapping a rigid four-cycle. The deformation to a generalized complex geometry is interpreted as a consequence of nonperturbative effects in the seven-brane gauge theory. We formulate the problem for seven-branes wrapping the base of an appropriate del Pezzo cone, and in the near-stack limit in which the four-cycle is flat, we obtain an exact solution in closed form. Our solutions serve to characterize the local geometry of nonperturbatively-stabilized flux compactifications.Comment: 49 pages, 2 figures; v2: minor corrections, references adde

    Critical and Non-Critical Einstein-Weyl Supergravity

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    We construct N=1 supersymmetrisations of some recently-proposed theories of critical gravity, conformal gravity, and extensions of critical gravity in four dimensions. The total action consists of the sum of three separately off-shell supersymmetric actions containing Einstein gravity, a cosmological term and the square of the Weyl tensor. For generic choices of the coefficients for these terms, the excitations of the resulting theory around an AdS_4 background describe massive spin-2 and massless spin-2 modes coming from the metric; massive spin-1 modes coming from a vector field in the theory; and massless and massive spin-3/2 modes (with two unequal masses) coming from the gravitino. These assemble into a massless and a massive N=1 spin-2 multiplet. In critical supergravity, the coefficients are tuned so that the spin-2 mode in the massive multiplet becomes massless. In the supersymmetrised extensions of critical gravity, the coefficients are chosen so that the massive modes lie in a "window" of lowest energies E_0 such that these ghostlike fields can be truncated by imposing appropriate boundary conditions at infinity, thus leaving just positive-norm massless supergravity modes.Comment: 29 page

    Teaching computer language handling - From compiler theory to meta-modelling

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    Most universities teach computer language handling by mainly focussing on compiler theory, although MDA (model-driven architecture) and meta-modelling are increasingly important in the software industry as well as in computer science. In this article, we investigate how traditional compiler theory compares to meta-modelling with regard to formally defining the different aspects of a language, and how we can expand the focus in computer language handling courses to also include meta-model-based approaches. We give an outline of a computer language handling course that covers both paradigms, and share some experiences from running a course based on this outline at the University of Agder
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