293 research outputs found

    Role of cytoskeletal remodeling in T cell receptor signaling and integrin activation at the immunological synapse

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    The efficiency of an immune response critically depends on the ability of T cells to respond to antigens. Upon encountering cognate antigenic peptides on the surface of antigen-presenting cells, T cells form a specialized interface, termed the immunological synapse (IS), which serves as the site of information transfer between the cells. This contact zone is characterized by the enrichment of signaling receptors, kinases and adaptor proteins, and is the site of extensive cytoskeletal remodeling. The versatile nature and spatio-temporal regulation of signaling cascades at the IS has long been recognized but the exact mechanisms that coordinate these processes remain poorly understood. In this work we have investigated the role of cytoskeletal remodeling in propagation of signaling events that lead to T cell activation. Using human T cell lines and primary T cells, we demonstrate that F-actin flow is largely driven by actin polymerization, rather than by myosin IIA contraction. While myosin IIA is able to exert forces on the cytoskeleton, it is dispensable for bulk network flow. Conversely, myosin IIA controls the extent of cell spreading and synaptic symmetry. We have also found that ongoing retrograde flow of F-actin sustains calcium mobilization at the level of release from endoplasmic reticulum stores. This defect is likely due to loss of PLCgamma1 activity at the IS, since the concentration of phosphorylated PLCgamma1 plummets upon F-actin immobilization. Furthermore, we have examined whether F-actin remodeling is required for integrin LFA-1 activation, which in turn strengthens conjugate formation and costimulation. Taking advantage of stimulatory planar lipid bilayers and cell-cell conjugates, we show that F-actin flow drives affinity maturation and spatial organization of LFA-1 at the IS. These observations are in line with a mechanotransduction model, in which F-actin-derived force induces integrin conformational change, thereby modulating binding affinity for ligand. The net inward movement of F-actin also recruits LFA-1 to the interface, thereby increasing its effective concentration. Taken together, these findings indicate that ongoing remodeling of actin cytoskeleton is required to sustain signaling and to choreograph spatio-temporal organization of receptors and their associated complexes at the IS during early phases of T cell activation

    Π ΠžΠ—Π ΠžΠ‘ΠšΠ Π Π•Π¦Π•ΠŸΠ’Π£Π Π˜ Π–Π˜Π ΠžΠ’ΠžΠ‡ НАЧИНКИ Π”Π›Π― ΠΠžΠ’ΠžΠ“Πž Π’Π˜Π”Π£ Π’ΠΠ€Π•Π›Π¬ΠΠ˜Π₯ Π’Π˜Π ΠžΠ‘Π†Π’

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    The article gives an opportunity to develop the technology of fatty filling for waffles and low-calorie wafers by replacing sugar with a mixture of sweet extracts from the leaves of stevia with erythritol. The expediency of regulating the amount of dry matter due to the introduction of dry skim milk whey has been proved. The whey is a raw material component that further enriches the finished product on minerals and vitamins that are healthy for the human body. The possibility of additional introduction of of beta-carotene, as a dye and ascorbic acid, as a stabilizer of fatty wafer fillings has been investigated. In order to improve the quality and safety of finished products, the possibility of using in the technology of fatty fillings for wafer products a new type of confectionery fat of domestic production "Fettifil" has been experimentally confirmed.Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΡ€ΠΈΠ²Π΅Π΄Π΅Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΆΠΈΡ€ΠΎΠ²ΠΎΠΉ Π½Π°Ρ‡ΠΈΠ½ΠΊΠΈ для Π²Π°Ρ„Π΅Π»ΡŒ ΠΈ Π²Π°Ρ„Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ ΠΏΠΎΠ½ΠΈΠΆΠ΅Π½Π½ΠΎΠΉ калорийности Π·Π° счСт Π·Π°ΠΌΠ΅Π½Ρ‹ сахара Π½Π° смСсь экстракта сладкого ΠΈΠ· Π»ΠΈΡΡ‚ΡŒΠ΅Π² стСвии с Π΅Ρ€ΠΈΡ‚Ρ€ΠΎΡ‚ΠΎΠ»ΠΎΠΌ. Π”ΠΎΠΊΠ°Π·Π°Π½Π° Ρ†Π΅Π»Π΅ΡΠΎΠΎΠ±Ρ€Π°Π·Π½ΠΎΡΡ‚ΡŒ рСгуляции количСства сухих вСщСств Π·Π° счСт внСсСния ΠΎΠ±Π΅Π·ΠΆΠΈΡ€Π΅Π½Π½ΠΎΠΉ ΠΌΠΎΠ»ΠΎΡ‡Π½ΠΎΠΉ сыворотки, ΠΊΠ°ΠΊ ΡΡ‹Ρ€ΡŒΠ΅Π²ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π°, которая Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΎΠ±ΠΎΠ³Π°Ρ‚ΠΈΡ‚ Π³ΠΎΡ‚ΠΎΠ²Ρ‹ΠΉ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ ΠΏΠΎΠ»Π΅Π·Π½Ρ‹ΠΌΠΈ для ΠΎΡ€Π³Π°Π½ΠΈΠ·ΠΌΠ° Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ° ΠΌΠΈΠ½Π΅Ρ€Π°Π»Π°ΠΌΠΈ ΠΈ Π²ΠΈΡ‚Π°ΠΌΠΈΠ½Π°ΠΌΠΈ. ИсслСдована Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ внСсСния Π±Π΅Ρ‚Π°-ΠΊΠ°Ρ€ΠΎΡ‚ΠΈΠ½Π°, Π² качСствС краситСля ΠΈ аскорбиновой кислоты, Π² качСствС стабилизатора ΠΆΠΈΡ€ΠΎΠ²Ρ‹Ρ… Π²Π°Ρ„Π΅Π»ΡŒΠ½Ρ‹Ρ… Π½Π°Ρ‡ΠΈΠ½ΠΎΠΊ. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ использования Π½ΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΈΠ΄Π° кондитСрского ΠΆΠΈΡ€Π° отСчСствСнного производства "Π€Π΅Ρ‚Ρ‚ΠΈΡ„ΠΈΠ»" Π² Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΆΠΈΡ€ΠΎΠ²Ρ‹Ρ… Π½Π°Ρ‡ΠΈΠ½ΠΎΠΊ для Π²Π°Ρ„Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ с Ρ†Π΅Π»ΡŒΡŽ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡ качСства ΠΈ бСзопасности Π³ΠΎΡ‚ΠΎΠ²ΠΎΠΉ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†ΠΈΠΈ.Π£ статті Π½Π°Π²Π΅Π΄Π΅Π½ΠΎ ΠΌΠΎΠΆΠ»ΠΈΠ²Ρ–ΡΡ‚ΡŒ Ρ€ΠΎΠ·Ρ€ΠΎΠ±ΠΊΠΈ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³Ρ–Ρ— ΠΆΠΈΡ€ΠΎΠ²ΠΎΡ— Π½Π°Ρ‡ΠΈΠ½ΠΊΠΈ для Π²Π°Ρ„Π΅Π»ΡŒ Ρ‚Π° Π²Π°Ρ„Π΅Π»ΡŒΠ½ΠΈΡ… Π²ΠΈΡ€ΠΎΠ±Ρ–Π² Π·Π½ΠΈΠΆΠ΅Π½ΠΎΡ— калорійності Π·Π° Ρ€Π°Ρ…ΡƒΠ½ΠΎΠΊ Π·Π°ΠΌΡ–Π½ΠΈ Ρ†ΡƒΠΊΡ€Ρƒ Π½Π° ΡΡƒΠΌΡ–Ρˆ Скстракту солодкого Π· листя стСвії Π· Π΅Ρ€ΠΈΡ‚Ρ€ΠΎΡ‚ΠΎΠ»ΠΎΠΌ. Π”ΠΎΠ²Π΅Π΄Π΅Π½Π° Π΄ΠΎΡ†Ρ–Π»ΡŒΠ½Ρ–ΡΡ‚ΡŒ рСгуляції ΠΊΡ–Π»ΡŒΠΊΠΎΡΡ‚Ρ– сухих Ρ€Π΅Ρ‡ΠΎΠ²ΠΈΠ½ Π·Π° Ρ€Π°Ρ…ΡƒΠ½ΠΎΠΊ внСсСння сухої ΠΌΠΎΠ»ΠΎΡ‡Π½ΠΎΡ— Π·Π½Π΅ΠΆΠΈΡ€Π΅Π½ΠΎΡ— сироватки, як сировинного ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Π°, Ρ‰ΠΎ Π΄ΠΎΠ΄Π°Ρ‚ΠΊΠΎΠ²ΠΎ Π·Π±Π°Π³Π°Ρ‚ΠΈΡ‚ΡŒ Π³ΠΎΡ‚ΠΎΠ²ΠΈΠΉ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ Π½Π° корисні для ΠΎΡ€Π³Π°Π½Ρ–Π·ΠΌΡƒ людини ΠΌΡ–Π½Π΅Ρ€Π°Π»ΠΈ Ρ‚Π° Π²Ρ–Ρ‚Π°ΠΌΡ–Π½ΠΈ. ДослідТСна ΠΌΠΎΠΆΠ»ΠΈΠ²Ρ–ΡΡ‚ΡŒ Π΄ΠΎΠ΄Π°Ρ‚ΠΊΠΎΠ²ΠΎΠ³ΠΎ внСсСння Π±Π΅Ρ‚Π°-ΠΊΠ°Ρ€ΠΎΡ‚ΠΈΠ½Ρƒ, Π² якості Π±Π°Ρ€Π²Π½ΠΈΠΊΠ° Ρ‚Π° аскорбінової кислоти, Π² якості стабілізатора ΠΆΠΈΡ€ΠΎΠ²ΠΈΡ… Π²Π°Ρ„Π΅Π»ΡŒΠ½ΠΈΡ… Π½Π°Ρ‡ΠΈΠ½ΠΎΠΊ. Π•ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ ΠΏΡ–Π΄Ρ‚Π²Π΅Ρ€Π΄ΠΆΠ΅Π½Π° ΠΌΠΎΠΆΠ»ΠΈΠ²Ρ–ΡΡ‚ΡŒ використання  Π½ΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΈΠ΄Ρƒ ΠΊΠΎΠ½Π΄ΠΈΡ‚Π΅Ρ€ΡΡŒΠΊΠΎΠ³ΠΎ ΠΆΠΈΡ€Ρƒ вітчизняного Π²ΠΈΡ€ΠΎΠ±Π½ΠΈΡ†Ρ‚Π²Π° "Π€Π΅Ρ‚Ρ‚Ρ–Ρ„Ρ–Π»" Ρƒ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³Ρ–Ρ— ΠΆΠΈΡ€ΠΎΠ²ΠΈΡ… Π½Π°Ρ‡ΠΈΠ½ΠΎΠΊ для Π²Π°Ρ„Π΅Π»ΡŒΠ½ΠΈΡ… Π²ΠΈΡ€ΠΎΠ±Ρ–Π² Π· ΠΌΠ΅Ρ‚ΠΎΡŽ підвищСння якості Ρ‚Π° Π±Π΅Π·ΠΏΠ΅ΠΊΠΈ Π³ΠΎΡ‚ΠΎΠ²ΠΎΡ— ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†Ρ–Ρ—

    Адсорбция Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄Π° Π½Π° чистых ΠΈ Π΄ΠΎΠΏΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½Ρ‹Ρ… Π½Π°Π½ΠΎΡ‚Ρ€ΡƒΠ±ΠΊΠ°Ρ…: DFT ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅

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    РассматриваСтся адсорбция Π½Π΅ΡΠΊΠΎΠ»ΡŒΠΊΠΈΡ… ΠΌΠΎΠ»Π΅ΠΊΡƒΠ» Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄Π° Π½Π° внСшнСй ΠΈ Π²Π½ΡƒΡ‚Ρ€Π΅Π½Π½Π΅ΠΉ повСрхности комплСкса "углСродная Π½Π°Π½ΠΎΡ‚Ρ€ΡƒΠ±ΠΊΠ° (9,9)@Li". ЧислСнныС экспСримСнты ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡŒ Π² ΠΏΠ°ΠΊΠ΅Ρ‚Π΅ SIESTA Π² Π΄Π²ΡƒΡ… приблиТСниях для ΠΎΠ±ΠΌΠ΅Π½Π½ΠΎ-коррСляционного ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»Π°: ΠΏΡ€ΠΈΠ±Π»ΠΈΠΆΠ΅Π½ΠΈΠΈ ΠΎΠ±ΠΎΠ±Ρ‰Π΅Π½Π½Ρ‹Ρ… Π³Ρ€Π°Π΄ΠΈΠ΅Π½Ρ‚ΠΎΠ² (GGA) ΠΈ ΠΏΡ€ΠΈΠ±Π»ΠΈΠΆΠ΅Π½ΠΈΠΈ локальной элСктронной плотности (LDA). ΠœΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ, Ρ‡Ρ‚ΠΎ Π΄ΠΎΠ±Π°Π²Π»Π΅Π½ΠΈΠ΅ Π°Ρ‚ΠΎΠΌΠ° лития позволяСт ΡƒΠ²Π΅Π»ΠΈΡ‡ΠΈΡ‚ΡŒ ΡΠ½Π΅Ρ€Π³ΠΈΡŽ адсорбции 3-4 ΠΌΠΎΠ»Π΅ΠΊΡƒΠ» Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄Π° (располоТСнных Π² ΠΏΠ΅Ρ€Π²ΠΎΠΉ ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ сфСрС Li) ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ со случаСм сорбции Π½Π° чистой повСрхности ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½ΠΎΠΉ Π½Π°Π½ΠΎΡ‚Ρ€ΡƒΠ±ΠΊΠΈ. ΠŸΡ€ΠΈ этом энСргии связи ΠΏΠΎΠΏΠ°Π΄Π°ΡŽΡ‚ Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½ 200-700 мэВ/(ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Ρƒ Н[2]), ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΠΉ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ Ρ†ΠΈΠΊΠ»ΠΎΠ² сорбции/дСсорбции Π³Π°Π·Π°, Ρ‚ΠΎΠ»ΡŒΠΊΠΎ Π² случаС Π²Π½ΡƒΡ‚Ρ€Π΅Π½Π½Π΅ΠΉ сорбции

    Анализ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½ΠΎΠ³ΠΎ обСспСчСния для Ρ‚Ρ€Π΅Ρ…ΠΌΠ΅Ρ€Π½ΠΎΠ³ΠΎ модСлирования ΠΈ ΠΎΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ мСстороТдСний Π½Π΅Ρ„Ρ‚ΠΈ ΠΈ Π³Π°Π·Π°

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    ΠΠ½Π°Π»ΠΈΠ·ΠΈΡ€ΡƒΡŽΡ‚ΡΡ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ распространСнныС Π½Π° Ρ€Ρ‹Π½ΠΊΠ΅ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½ΠΎΠ³ΠΎ обСспСчСния срСдства ΠΈ комплСксы, примСняСмыС Π² России ΠΈ Π·Π° Ρ€ΡƒΠ±Π΅ΠΆΠΎΠΌ для ΠΈΠ½Ρ‚Π΅Ρ€ΠΏΡ€Π΅Ρ‚Π°Ρ†ΠΈΠΈ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² исслСдований ΠΈ создания Ρ†ΠΈΡ„Ρ€ΠΎΠ²Ρ‹Ρ… 3D-ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ мСстороТдСний Π½Π΅Ρ„Ρ‚ΠΈ ΠΈ Π³Π°Π·Π°. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ тСхнологичСскиС Π»ΠΈΠ½Π΅ΠΉΠΊΠΈ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½Ρ‹Ρ… ΠΌΠΎΠ΄ΡƒΠ»Π΅ΠΉ, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΠ΅ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΈΠ΅ всСго комплСкса Ρ€Π°Π±ΠΎΡ‚ ΠΏΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡŽ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ мСстороТдСний. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ‹ авторскиС ΠΈΠ½ΡΡ‚Ρ€ΡƒΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ срСдства (алгоритмичСскиС ΠΈ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½Ρ‹Π΅) для ΠΎΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ процСсса модСлирования Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ мСстороТдСний Π½Π΅Ρ„Ρ‚ΠΈ ΠΈ Π³Π°Π·Π°. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Π°Π½Π°Π»ΠΈΠ·Π° ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ Π°Ρ€Π³ΡƒΠΌΠ΅Π½Ρ‚ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ Π²Ρ‹Π±ΠΎΡ€ Ρ€Π°Ρ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π½Π°Π±ΠΎΡ€Π° ΠΈΠ½ΡΡ‚Ρ€ΡƒΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… срСдств ΠΈΠ· арсСнала российского ΠΈ Π·Π°Ρ€ΡƒΠ±Π΅ΠΆΠ½ΠΎΠ³ΠΎ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½ΠΎΠ³ΠΎ обСспСчСния

    A spatial contrast retina with on-chip calibration for neuromorphic spike-based AER vision systems

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    We present a 32 32 pixels contrast retina microchip that provides its output as an address event representation (AER) stream. Spatial contrast is computed as the ratio between pixel photocurrent and a local average between neighboring pixels obtained with a diffuser network. This current-based computation produces an important amount of mismatch between neighboring pixels, because the currents can be as low as a few pico-amperes. Consequently, a compact calibration circuitry has been included to trimm each pixel. Measurements show a reduction in mismatch standard deviation from 57% to 6.6% (indoor light). The paper describes the design of the pixel with its spatial contrast computation and calibration sections. About one third of pixel area is used for a 5-bit calibration circuit. Area of pixel is 58 m 56 m, while its current consumption is about 20 nA at 1-kHz event rate. Extensive experimental results are provided for a prototype fabricated in a standard 0.35- m CMOS process.This work was supported by Spanish Research Grants TIC2003-08164-C03-01 (SAMANTA), TEC2006-11730-C03-01 (SAMANTA-II), and EU grant IST-2001-34124 (CAVIAR). JCS was supported by the I3P program of the Spanish Research Council. RSG was supported by a national grant from the Spanish Ministry of Education and Science.Peer reviewe

    Testing the Randall-Sundrum Model at a High Energy eβˆ’eβˆ’e^- e^- Collider

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    We study the process eβˆ’eβˆ’β†’eβˆ’eβˆ’e^- e^- \to e^- e^- at a high energy eβˆ’eβˆ’e^- e^- collider including the effect of graviton exchanges in the warped gravity model of Randall and Sundrum. Discovery limits for gravitons are established and the effects of polarization are discussed.Comment: 10 pages LaTeX, 6 postscript figure

    Influence of torrefaction on the grindability and reactivity of woody biomass

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    7 pages, 5 figures, 4 tables.-- Available online Oct 23, 2007.The use of biomass to produce energy is becoming more and more frequent as it helps to achieve a sustainable environmental scenario. However the exploitation of this fuel source does have drawbacks that need to be solved. In this work, the torrefaction of woody biomass (eucalyptus) was studied in order to improve its properties for pulverised systems. The process consisted in a heating treatment at moderate temperature (240, 260, 280Β°C) under an inert atmosphere. The grindability of raw biomass and the treated samples was compared and an improvement in the grindability characteristics was observed after the torrefaction process. Thermogravimetric analysis of the samples was carried out in order to study their reactivity in air. The DTG curves of the torrefied biomass showed a double peak nature. The kinetic parameters were calculated for each reaction stage. The torrefaction process was found to influence the parameters of the first stage, whereas those corresponding to the second remained unaffected.This work was carried out with financial support from the Spanish CDTI (Project CENIT PiIBE) and ELCOGAS, S.A. M.G.P. and C.P. acknowledge the support from the CSIC I3P Program co-financed by the European Social Fund, and J.F. from the Plan Regional de Investigacion del Principado de Asturias.Peer reviewe

    Thermal non-Gaussianity in holographic cosmology

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    Recently it has been shown that the thermal holographic fluctuations can give rise to an almost scale invariant spectrum of metric perturbations since in this scenario the energy is proportional to the area of the boundary rather than the volume. Here we calculate the non-Gaussianity of the spectrum of cosmological fluctuations in holographic phase, which can imprint on the radiation dominated universe by an abrupt transition. We find that if the matter is phantom-like, the non-Gaussianity fNLequilf_{NL}^{equil} can reach O(1){\cal O}(1) or even be larger than O(1){\cal O}(1). Especially in the limit Ο‰β†’βˆ’5/3\omega\to -5/3, the non-Gaussianity is very large and negative. Furthermore, since the energy is proportional to the area, the thermal holographic non-Gaussianity depends linearly on kk if we neglect the variation in TT during the transition (fixed temperature).Comment: 13 pages, Minor corrections and one reference added;v3,minor correction

    Thermal fluctuations in viscous cosmology

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    In this paper we investigate the power spectrum of thermal fluctuations in very early stage of viscous cosmology. When the state parameter as well as the viscous coefficient of a barotropic fluid is properly chosen, a scale invariant spectrum with large non-Gaussianity can be obtained. In contrast to the results previously obtained in string gas cosmology and holographic cosmology, we find the non-Gaussianity in this context can be k-independent such that it is not suppressed at large scale, which is expected to be testified in future observation.Comment: 13 pages, no figure, typos corrected, references adde
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