964 research outputs found
Phase Space Tomography of Matter-Wave Diffraction in the Talbot Regime
We report on the theoretical investigation of Wigner distribution function
(WDF) reconstruction of the motional quantum state of large molecules in de
Broglie interference. De Broglie interference of fullerenes and as the like
already proves the wavelike behaviour of these heavy particles, while we aim to
extract more quantitative information about the superposition quantum state in
motion. We simulate the reconstruction of the WDF numerically based on an
analytic probability distribution and investigate its properties by variation
of parameters, which are relevant for the experiment. Even though the WDF
described in the near-field experiment cannot be reconstructed completely, we
observe negativity even in the partially reconstructed WDF. We further consider
incoherent factors to simulate the experimental situation such as a finite
number of slits, collimation, and particle-slit van der Waals interaction. From
this we find experimental conditions to reconstruct the WDF from Talbot
interference fringes in molecule Talbot-Lau interferometry.Comment: 16 pages, 9 figures, accepted at New Journal of Physic
Giant Liquid Argon Observatory for Proton Decay, Neutrino Astrophysics and CP-violation in the Lepton Sector (GLACIER)
GLACIER (Giant Liquid Argon Charge Imaging ExpeRiment) is a large underground
observatory for proton decay search, neutrino astrophysics and CP-violation
studies in the lepton sector. Possible underground sites are studied within the
FP7 LAGUNA project (Europe) and along the JPARC neutrino beam in collaboration
with KEK (Japan). The concept is scalable to very large masses.Comment: 4 pages, 1 figure, Contribution to the Workshop "European Strategy
for Future Neutrino Physics", CERN, Oct. 200
ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π½Π΅ΠΉΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ Π΄Π΅ΡΠ΅ΠΊΡΠΎΡΠ° ΠΈΠ· ΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠ° o100?200 ΠΌΠΌ
Π Π°ΡΡΡΠΈΡΡΠ²Π°Π΅ΡΡΡ ΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΠΎ ΠΏΡΠΎΠ²Π΅ΡΡΠ΅ΡΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ Π΄Π΅ΡΠ΅ΠΊΡΠΎΡΠ°. ΠΊ Π½Π΅ΠΉΡΡΠΎΠ½Π°ΠΌ ΡΠ²Π΅ΡΡ
Π²ΡΡΠΎΠΊΠΈΡ
(Π΄Π΅ΡΡΡΠΊΠΈ ΠΈ ΡΠΎΡΠ½ΠΈ ΠΡΠ) ΡΠ½Π΅ΡΠ³ΠΈΠΉ
The interlayer cohesive energy of graphite from thermal desorption of polyaromatic hydrocarbons
We have studied the interaction of polyaromatic hydrocarbons (PAHs) with the
basal plane of graphite using thermal desorption spectroscopy. Desorption
kinetics of benzene, naphthalene, coronene and ovalene at sub-monolayer
coverages yield activation energies of 0.50 eV, 0.85 eV, 1.40 eV and 2.1 eV,
respectively. Benzene and naphthalene follow simple first order desorption
kinetics while coronene and ovalene exhibit fractional order kinetics owing to
the stability of 2-D adsorbate islands up to the desorption temperature.
Pre-exponential frequency factors are found to be in the range
- as obtained from both Falconer--Madix (isothermal
desorption) analysis and Antoine's fit to vapour pressure data. The resulting
binding energy per carbon atom of the PAH is 5 meV and can be identified
with the interlayer cohesive energy of graphite. The resulting cleavage energy
of graphite is ~meV/atom which is considerably larger than previously
reported experimental values.Comment: 8 pages, 4 figures, 2 table
Development of molecularly imprinted polymer membranes with specificity to triazine herbicides, prepared by the "surface photografting" technique
Β«Surface photograftingΒ» of polypropylene (PPy) microporous membranes by molecularly imprinted polymers selective to triazine herbicides has been carried out by the UV irradiation-initiated co-polymerization of the functional monomer (2-acrylamido-2-methyl-1-propane sulphonic acid) and a cross-linker (N,N?-methylene-bis-acrylamide) in the presence of the template (terbumeton) onto photoinitiator (benzophenone)-coated samples. The grafting reaction occurs in a thin liquid layer on the membrane substrate, which is pre-soaked in a dimethyl formamide solution containing template, functional monomer and cross-linker. After irradiation with a 500 W mercury lamp for 10 min at room temperature, the membranes covered with the layer of imprinted polymer were obtained. The recognition sites complementary to terbumeton were formed in the membranes after extraction of the template molecules with methanol. Alternatively, reference polymeric membranes were prepared with the same monomer composition, but without the template. The membranes' recognition properties were estimated by their capability to herbicide adsorption from its aqueous solution. The membranes modified by the mixture of monomers containing terbumeton showed significantly higher adsorption capability to this herbicide than to analogous compounds (terbuthylazine, atrazine, desmetryn, metribuzine). The effect of the polymer composition on the binding properties of the membranes has been investigated. High affinity of these membranes to triazine herbicides together with their inexpensive preparation, provide a good basis for applications of molecularly imprinted polymer membranes in separation and solid-phase extraction.Π‘ΠΈΠ½ΡΠ΅Π·ΠΎΠ²Π°Π½ΠΎ Π½ΠΎΠ²ΠΈΠΉ ΡΠΈΠΏ ΠΌΠ°ΡΡΠΈΡΠ½ΠΈΡ
ΠΏΠΎΠ»ΡΠΌΠ΅ΡΠ½ΠΈΡ
ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ ΡΠ»ΡΒΡ
ΠΎΠΌ ΠΏΠΎΠ²Π΅ΡΡ
Π½Π΅Π²ΠΎΡ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠ°ΡΡΡ ΠΌΡΠΊΡΠΎΡΡΠ»ΡΡΡΠ°ΡΡΠΉΠ½ΠΈΡ
ΠΏΠΎΠ»ΡΠΏΡΠΎΠΏΡΒ Π»Π΅Π½ΠΎΠ²ΠΈΡ
ΠΌΠ΅ΠΌΠ±ΡΠ°Π½, ΡΠΊΠ° ΠΏΠΎΠ»ΡΠ³Π°Π»Π° Π² Π½Π°Π½Π΅ΡΠ΅Π½Π½Ρ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½Ρ ΡΠΎΠ½ΠΊΠΎΠ³ΠΎ ΡΠ°ΡΡ ΠΌΠ°ΡΡΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»ΡΠΌΠ΅ΡΡ, ΡΠ΅Π»Π΅ΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π΄ΠΎ ΡΡΠΈΠ°Π·ΠΈΠ½ΠΎΠ²ΠΎΠ³ΠΎ Π³Π΅ΡΠ±ΡΡΠΈΠ΄Ρ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ. ΠΠ°ΡΡΠΈΡΠ½Ρ ΠΏΠΎΠ»ΡΠΌΠ΅ΡΠΈΠ·Π°ΡΡΡ Π·Π΄ΡΠΉΡΠ½ΡΠ²Π°Π»ΠΈ Π² Π΄ΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΎΡΠΌΠ°ΠΌΡΠ΄Ρ, Π²ΠΈΠΊΠΎΡΠΈΡΡΠΎΠ²ΡΡΡΠΈ Π³Π΅ΡΠ±ΡΡΠΈΠ΄ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½ ΡΠΊ ΠΌΠ°ΡΡΠΈΡΡ, 2-Π°ΠΊΡΠΈΠ»Π°ΠΌΡΠ΄ΠΎ-2-ΠΌΠ΅ΡΠΈΠ»-1-ΠΏΡΠΎΠΏΠ°Π½-ΡΡΠ»ΡΡΠΎΠ½ΠΎΠ²Ρ Π ΠΌΠ΅ΡΠ°ΠΊΡΠΈΠ»ΠΎΠ²Ρ Π Π°ΠΊΡΠΈΠ»ΠΎΠ²Ρ ΠΊΠΈΡΠ»ΠΎΡΡ ΡΠΊ ΡΡΠ½ΠΊΡΡΠΎΠ½Π°Π»ΡΠ½ΠΈΠΉ ΠΌΠΎΠ½ΠΎΠΌΠ΅Ρ Ρ N ,N' -ΠΌΠ΅ΡΠΈΠ»Π΅Π½-Π±ΡΡΠ°ΠΊΡΠΈΠ»Π°ΠΌΡΠ΄ ΡΠΊ Π·ΡΠΈΠ²Π°Π»ΡΠ½ΠΈΠΉ Π°Π³Π΅Π½Ρ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½Ρ ΠΌΡΠΊΡΠΎΡΡΠ»ΡΡΡΠ°ΡΡΠΉΠ½ΠΎΡ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ΠΈ, ΠΏΠΎΠΊΡΠΈΡΠΎΡ ΡΠΎΠ½ΠΊΠΈΠΌ ΡΠ°ΒΡΠΎΠΌ ΡΠΎΡΠΎΡΠ½ΡΡΡΠΈΡΠΎΡΠ° Π±Π΅Π½Π·ΠΎΡΠ΅Π½ΠΎΠ½Ρ. ΠΠΊΡΡΡΠ°ΠΊΡΡΡ ΠΌΠ°ΡΡΠΈΡΠ½ΠΈΡ
ΠΌΠΎΒΠ»Π΅ΠΊΡΠ» ΡΠΏΡΠΈΡΠΈΠ½ΡΠ²Π°Π»Π° ΡΠΎΡΠΌΡΠ²Π°Π½Π½Ρ Π² ΡΡΡΡΠΊΡΡΡΡ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ΠΈ ΡΠ°ΠΉΒΡΡΠ², ΡΠΊΡ Π·Π° ΡΠΎΡΠΌΠΎΡ ΡΠ° ΠΏΡΠΎΠ΅ΠΏΡΡΠΎΠ²ΠΈΠΌ ΡΠΎΠ·ΡΠ°ΡΡΠ²Π°Π½Π½ΡΠΌ ΡΡΠ½ΠΊΒΡΡΠΎΠ½Π°Π»ΡΠ½ΠΈΡ
Π³ΡΡΠΏ Π±ΡΠ»ΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½ΠΈΠΌΠΈ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ. ΠΠΎΠ½ΡΒΡΠΎΠ»ΡΠ½Ρ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ΠΈ ΠΌΠΎΠ΄ΠΈΡΡΠΊΡΠ²Π°Π»ΠΈ Π· Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½ΡΠΌ ΠΏΠΎΠ΄ΡΠ±Π½ΠΎΡ ΡΡΒΠΌΡΡΡ ΠΌΠΎΠ½ΠΎΠΌΠ΅ΡΡΠ², ΡΠΎ Π½Π΅ ΠΌΡΡΡΠΈΠ»Π° ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ. ΠΠ΄Π°ΡΠ½ΡΡΡΡ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ Π΄ΠΎ ΡΠ΅Π»Π΅ΠΊΡΠΈΠ²Π½ΠΎΡ Π°Π΄ΡΠΎΡΠ±ΡΡΡ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½ΠΎ Π² Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ Π²ΡΠ΄ ΡΠΈΠΏΡ ΡΠ° ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΡΡ ΡΡΠ½ΠΊΡΡΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΌΠΎΠ½ΠΎΒΠΌΠ΅ΡΠ°, Π° ΡΠ°ΠΊΠΎΠΆ Π²ΡΠ΄ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΡΡ Π·ΡΠΈΠ²Π°Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π³Π΅Π½ΡΠ° Π² ΠΌΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΡΠΉ ΡΡΠΌΡΡΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΠΎ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½-ΡΠΌΠΏΡΠΈΠ½ΡΠΎΠ²Π°Π½Ρ ΠΌΠ°ΡΒΡΠΈΡΠ½Ρ ΠΏΠΎΠ»ΡΠΌΠ΅ΡΠ½Ρ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΡΡΡΡΡ Π²ΠΈΡΠΎΠΊΠΎΡ ΡΠ΅Π»Π΅ΠΊΒΡΠΈΠ²Π½ΡΡΡΡ ΡΡΠΎΡΠΎΠ²Π½ΠΎ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ ΡΠ° Π·Π΄Π°ΡΠ½ΡΡΡΡ Π΄ΠΎ Π½Π΅Π·Π½Π°ΡΠ½ΠΎΡ Π°Π΄ΡΠΎΡΠ±ΡΡΡ ΠΉΠΎΠ³ΠΎ ΡΡΡΡΠΊΡΡΡΠ½ΠΈΡ
Π°Π½Π°Π»ΠΎΠ³ΡΠ² β ΡΠ΅ΡΡΠ±ΡΡΠΈΠ»Π°Π·ΠΈΠ½Ρ, Π°ΡΡΠ°Π·ΠΈΠ½Ρ, Π΄Π΅ΡΠΌΠ΅ΡΡΠΈΠ½Ρ Ρ ΠΌΠ΅ΡΡΠΈΠ±ΡΠ·ΠΈΠ½Ρ. Π’Π°ΠΊΡ Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΡ ΡΠΈΠ½ΡΠ΅Π·ΠΎΒΠ²Π°Π½ΠΈΡ
ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ Π·Π°Π±Π΅Π·ΠΏΠ΅ΡΡΡΡΡ ΡΡ
Π½Ρ Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½Π΅ Π²ΠΈΠΊΠΎΡΠΈΡΡΠ°Π½Π½Ρ Ρ ΡΠ²Π΅ΡΠ΄ΠΎΡΠ°Π·ΠΎΠ²ΡΠΉ Π΅ΠΊΡΡΡΠ°ΠΊΡΡΡ.Π‘ΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ Π½ΠΎΠ²ΡΠΉ ΡΠΈΠΏ ΠΌΠ°ΡΡΠΈΡΠ½ΡΡ
ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ½ΡΡ
ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΠΎΠΉ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΠΌΠΈΠΊΡΠΎΡΠΈΠ»ΡΡΡΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΠΎΠ»ΠΈΠΏΡΠΎΠΏΠΈΠ»Π΅Π½ΠΎΠ²ΡΡ
ΠΌΠ΅ΠΌΠ±ΡΠ°Π½, Π·Π°ΠΊΠ»ΡΡΠ°ΡΡΠ΅ΠΌΡΡ Π² Π½Π°Π½Π΅ΡΠ΅Π½ΠΈΠΈ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡ ΡΠΎΠ½ΠΊΠΎΠ³ΠΎ ΡΠ»ΠΎΡ ΠΌΠ°ΡΡΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ°, ΡΠ΅Π»Π΅ΠΊΡΠΈΠ²Π½ΠΎΒΠ³ΠΎ ΠΊ ΡΡΠΈΠ°Π·ΠΈΠ½ΠΎΠ²ΠΎΠΌΡ Π³Π΅ΡΠ±ΠΈΡΠΈΠ΄Ρ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ. ΠΠ°ΡΡΠΈΡΠ½ΡΡ ΠΏΠΎΠ»ΠΈΒΠΌΠ΅ΡΠΈΠ·Π°ΡΠΈΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π² Π΄ΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΎΡΠΌΠ°ΠΌΠΈΠ΄Π΅ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΡΠΈΠ°Π·ΠΈΠ½ΠΎΠ²ΠΎΠ³ΠΎ Π³Π΅ΡΠ±ΠΈΡΠΈΠ΄Π° ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Π° Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΌΠ°ΡΡΠΈΡΡ, 2-Π°ΠΊΡΠΈΠ»Π°ΠΌΠΈΠ΄ΠΎ-2-ΠΌΠ΅ΡΠΈΠ»-1-ΠΏΡΠΎΠΏΠ°Π½-ΡΡΠ»ΡΡΠΎΠ½ΠΎΠ²ΠΎΠΉΡ ΠΌΠ΅ΡΠ°ΠΊΡΠΈΠ»ΠΎΠ²ΠΎΠΉ Π°ΠΊΡΠΈΠ»ΠΎΠ²ΠΎΠΉ ΠΊΠΈΡΠ»ΠΎΡΡ ΠΊΠ°ΠΊ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΌΠΎΠ½ΠΎΠΌΠ΅ΡΠ° ΠΈ N,N'-ΠΌΠ΅ΡΠΈΠ»Π΅Π½-Π±ΠΈ ΡΠ°ΠΊ ΡΠΈΠ»Π°ΠΌ ΠΈΠ΄Π° ΠΊΠ°ΠΊ ΡΡΠΈΠ²Π°ΡΡΠ΅Π³ΠΎ Π°Π³Π΅Π½ΠΏΡ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΌΠΈΠΊΡΠΎΡΠΈΠ»ΡΡΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½Ρ, ΠΏΠΎΠΊΡΡΡΠΎΠΉ ΡΠΎΠ½ΠΊΠΈΠΌ ΡΠ»ΠΎΠ΅ΠΌ ΡΠΎΡΠΎΠΈΠ½ΠΈΠΈΡΡΡΡΠ° Π±Π΅Π½Π·ΠΎΡΠ΅Π½ΠΎΠ½Π°. ΠΠΊΡΡΡΠ°ΠΊΡΠΈΡ ΠΌΠ°ΡΡΠΈΡΠ½ΡΡ
ΠΌΠΎΠ»Π΅ΒΠΊΡΠ» ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΠ»Π° ΠΊ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π² ΡΡΡΡΠΊΡΡΡΠ΅ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½Ρ ΡΠ°ΠΉΒΡΠΎΠ², ΠΊΠΎΠΌΠΏΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½ΡΡ
ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ ΠΏΠΎ ΡΠΎΡΠΌΠ΅ ΠΈ ΠΏΡΠΎΡΡΡΠ°Π½ΒΡΡΠ²Π΅Π½Π½ΠΎΠΌΡ ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΡ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
Π³ΡΡΠΏΠΏ. ΠΠΎΠ½ΡΡΠΎΠ»ΡΒ Π½ΡΠ΅ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½Ρ ΡΠΈΠ½ΡΠ΅Π·ΠΎΡΠΎΠ²Π°Π»ΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΎΠΉ ΠΆΠ΅ ΠΌΠΎΠ½ΠΎΒΠΌΠ΅ΡΠ½ΠΎΠΉ ΡΠΌΠ΅ΡΠΈ Π² ΠΎΡΡΡΡΡΡΠ²ΠΈΠ΅ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Π°. Π‘ΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡ ΠΌΠ΅ΠΌΒ Π±ΡΠ°Π½ ΠΊ ΡΠ΅Π»Π΅ΠΊΡΠΈΠ²Π½ΠΎΠΉ Π°Π΄ΡΠΎΡΠ±ΡΠΈΠΈ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Π° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΠΈΠΏΠ° ΠΈ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΌΠΎΠ½ΠΎΒΠΌΠ΅ΡΠ°, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΡΡΠΈΠ²Π°ΡΡΠ΅Π³ΠΎ Π°Π³Π΅Π½ΡΠ°, Π² ΠΌΠΎΠ½ΠΎΠΌΠ΅ΡΒΠ½ΠΎΠΉ ΡΠΌΠ΅ΡΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½-ΠΈΠΌΠΏΡΠΈΠ½ΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ ΠΌΠ°ΡΡΠΈΡΠ½ΡΠ΅ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ½ΡΠ΅ ΠΌΠ΅ΠΌΠ±ΡΠ°Π½Ρ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΡΡΡΡ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΠ΅Π»Π΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ ΠΊ ΡΠ΅ΡΠ±ΡΠΌΠ΅ΡΠΎΠ½Ρ ΠΈ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΡΡ Π½Π΅Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ Π°Π΄ΡΠΎΡΠ±ΡΠΈΡ Π΅Π³ΠΎ ΡΡΡΡΠΊΡΡΡΠ½ΠΈΡ
Π°Π½Π°Π»ΠΎΠ³ΠΎΠ² β ΡΠ΅ΡΡΠ±ΡΡΠΈΠ»Π°Π·ΠΈΠ½Π°, Π°ΡΡΠ°Π·ΠΈΠ½Π°, Π΄Π΅ΡΠΌΠ΅ΡΡΠΈΠ½Π° ΠΈ ΠΌΠ΅ΡΡΠΈΠ±ΡΠ·ΠΈΠ½Π°. Π’Π°ΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΡΠΈΠ½ΡΠ΅Π·ΠΎΠ²Π°Π½Π½ΡΡ
ΠΌΠ΅ΠΌΠ±ΡΠ°Π½ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°ΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΠΈΡ
ΡΡΒΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π² ΡΠ²Π΅ΡΠ΄ΠΎΡΠ°Π·Π½ΠΎΠΉ ΡΠΊΡΡΡΠ°ΠΊΡΠΈΠΈ
Collision Dynamics and Solvation of Water Molecules in a Liquid Methanol Film
Environmental molecular beam experiments are used to examine water
interactions with liquid methanol films at temperatures from 170 K to 190 K. We
find that water molecules with 0.32 eV incident kinetic energy are efficiently
trapped by the liquid methanol. The scattering process is characterized by an
efficient loss of energy to surface modes with a minor component of the
incident beam that is inelastically scattered. Thermal desorption of water
molecules has a well characterized Arrhenius form with an activation energy of
0.47{\pm}0.11 eV and pre-exponential factor of 4.6 {\times} 10^(15{\pm}3)
s^(-1). We also observe a temperature dependent incorporation of incident water
into the methanol layer. The implication for fundamental studies and
environmental applications is that even an alcohol as simple as methanol can
exhibit complex and temperature dependent surfactant behavior.Comment: 8 pages, 5 figure
Application to the Analysis of Germinal Center Reactions In Vivo
Simultaneous detection of multiple cellular and molecular players in their
native environment, one of the keys to a full understanding of immune
processes, remains challenging for in vivo microscopy. Here, we present a
synergistic strategy for spectrally multiplexed in vivo imaging composed of
(i) triple two-photon excitation using spatiotemporal synchronization of two
femtosecond lasers, (ii) a broad set of fluorophores with emission ranging
from blue to near infrared, (iii) an effective spectral unmixing algorithm.
Using our approach, we simultaneously excite and detect seven fluorophores
expressed in distinct cellular and tissue compartments, plus second harmonics
generation from collagen fibers in lymph nodes. This enables us to visualize
the dynamic interplay of all the central cellular players during germinal
center reactions. While current in vivo imaging typically enables recording
the dynamics of 4 tissue components at a time, our strategy allows a more
comprehensive analysis of cellular dynamics involving 8 single-labeled
compartments. It enables to investigate the orchestration of multiple cellular
subsets determining tissue function, thus, opening the way for a mechanistic
understanding of complex pathophysiologic processes in vivo. In the future,
the design of transgenic mice combining a larger spectrum of fluorescent
proteins will reveal the full potential of our method
The ArDM experiment
The aim of the ArDM project is the development and operation of a one ton
double-phase liquid argon detector for direct Dark Matter searches. The
detector measures both the scintillation light and the ionization charge from
ionizing radiation using two independent readout systems. This paper briefly
describes the detector concept and presents preliminary results from the ArDM
R&D program, including a 3 l prototype developed to test the charge readout
system.Comment: Proceedings of the Epiphany 2010 Conference, to be published in Acta
Physica Polonica
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