نتایج جستجو برای: b0 no inoculation control

تعداد نتایج: 4292969  

Journal: :Mathematics 2022

Positivity analysis is used with some basic conditions to analyse monotonicity across all discrete fractional disciplines. This article addresses the of nabla differences Riemann–Liouville type by considering positivity ∇b0RLθg(z) combined a condition on g(b0+2), g(b0+3) and g(b0+4), successively. The ends relationship between integer type, which serves show difference ∇b0RLθg(z).

Journal: :Buildings 2022

Retrofitting measures in old buildings aimed at reducing energy usage have become important procedures meant to counteract the effects of climate change and greenhouse gas emissions. The aim this study is evaluate usage, thermal comfort, CO2 emissions an building by changing parameters such as orientation, shading systems, location, low film application, alternative supply form a geothermal hea...

2006
ARKADY BERENSTEIN Joseph Donin

For each reductive algebraic group G we introduce and study unipotent bicrystals which serve as a regular version of birational geometric and unipotent crystals introduced earlier by the authors. The framework of unipotent bicrystals allows, on the one hand, to study systematically such varieties as Bruhat cells in G and their convolution products and, on the other hand, to give a new construct...

Journal: :Pesquisa Agropecuaria Brasileira 2021

Abstract: The objective of this work was to evaluate the response BRS Tumucumaque cowpea (Vigna unguiculata) cultivar liming and phosphorus potassium fertilization in absence inoculation or nitrogen fertilization, as well with selected Bradyrhizobium strains, an upland forest area state Amapá, eastern Amazon, Brazil. Seven experiments were conducted field conditions, order six limestone, four p...

2009
Ivan Tkac

Adjustment of the static magnetic field homogeneity, commonly known as the B0 shimming or simply shimming, is essential for magnetic resonance spectroscopy because it determines the spectral resolution which is critical for reliable metabolite quantification. Inhomogeneities in the B0 field, resulting primarily from susceptibility differences between air and tissue, are scaled with the B0 field...

Journal: :Analytical biochemistry 2017
Christoph Juchem Robin A de Graaf

The homogenization of B0 conditions is necessary for every magnetic resonance spectroscopy (MRS) investigation. Its direct consequence is narrow spectral lines, on which reliable separation and quantification of biochemicals, and thus experimentally obtainable metabolic information, fundamentally relies. Besides spectral linewidth, unwanted B0 inhomogeneity also impairs other aspects of the MRS...

Journal: :Physical review letters 2006
D Acosta J Adelman T Affolder T Akimoto M G Albrow D Ambrose S Amerio D Amidei A Anastassov K Anikeev A Annovi J Antos M Aoki G Apollinari T Arisawa J-F Arguin A Artikov W Ashmanskas A Attal F Azfar P Azzi-Bacchetta N Bacchetta H Bachocou W Badgett A Barbaro-Galtieri G J Barker V E Barnes B A Barnett S Baroiant G Bauer F Bedeschi S Behari S Belforte G Bellettini J Bellinger A Belloni E Ben-Haim D Benjamin A Beretvas T Berry A Bhatti M Binkley D Bisello M Bishai R E Blair C Blocker K Bloom B Blumenfeld A Bocci A Bodek G Bolla A Bolshov D Bortoletto J Boudreau S Bourov B Brau C Bromberg E Brubaker J Budagov H S Budd K Burkett G Busetto P Bussey K L Byrum S Cabrera M Campanelli M Campbell F Canelli A Canepa M Casarsa D Carlsmith R Carosi S Carron M Cavalli-Sforza A Castro P Catastini D Cauz A Cerri L Cerrito J Chapman Y C Chen M Chertok G Chiarelli G Chlachidze F Chlebana I Cho K Cho D Chokheli J P Chou S Chuang K Chung W-H Chung Y S Chung M Cijliak C I Ciobanu M A Ciocci A G Clark D Clark M Coca A Connolly M Convery J Conway B Cooper K Copic M Cordelli G Cortiana J Cranshaw J Cuevas A Cruz R Culbertson C Currat D Cyr D Dagenhart S Da Ronco S D'Auria P de Barbaro S De Cecco A Deisher G De Lentdecker M Dell'Orso S Demers L Demortier M Deninno D Depedis P F Derwent C Dionisi J R Dittmann P DiTuro C Dörr A Dominguez S Donati M Donega J Donini M D'Onofrio T Dorigo K Ebina J Efron J Ehlers R Erbacher M Erdmann D Errede S Errede R Eusebi H-C Fang S Farrington I Fedorko W T Fedorko R G Feild M Feindt J P Fernandez R D Field G Flanagan L R Flores-Castillo A Foland S Forrester G W Foster M Franklin J C Freeman Y Fujii I Furic A Gajjar M Gallinaro J Galyardt M Garcia-Sciveres A F Garfinkel C Gay H Gerberich D W Gerdes E Gerchtein S Giagu P Giannetti A Gibson K Gibson C Ginsburg K Giolo M Giordani M Giunta G Giurgiu V Glagolev D Glenzinski M Gold N Goldschmidt D Goldstein J Goldstein G Gomez G Gomez-Ceballos M Goncharov O González I Gorelov A T Goshaw Y Gotra K Goulianos A Gresele M Griffiths C Grosso-Pilcher U Grundler J Guimaraes da Costa C Haber K Hahn S R Hahn E Halkiadakis A Hamilton B-Y Han R Handler F Happacher K Hara M Hare R F Harr R M Harris F Hartmann K Hatakeyama J Hauser C Hays H Hayward B Heinemann J Heinrich M Hennecke M Herndon C Hill D Hirschbuehl A Hocker K D Hoffman A Holloway S Hou M A Houlden B T Huffman Y Huang R E Hughes J Huston K Ikado J Incandela G Introzzi M Iori Y Ishizawa C Issever A Ivanov Y Iwata B Iyutin E James D Jang B Jayatilaka D Jeans H Jensen E J Jeon M Jones K K Joo S Y Jun T Junk T Kamon J Kang M Karagoz Unel P E Karchin Y Kato Y Kemp R Kephart U Kerzel V Khotilovich B Kilminster D H Kim H S Kim J E Kim M J Kim M S Kim S B Kim S H Kim Y K Kim M Kirby L Kirsch S Klimenko M Klute B Knuteson B R Ko H Kobayashi D J Kong K Kondo J Konigsberg K Kordas A Korn A Korytov A V Kotwal A Kovalev J Kraus I Kravchenko A Kreymer J Kroll M Kruse V Krutelyov S E Kuhlmann S Kwang A T Laasanen S Lai S Lami S Lammel M Lancaster R Lander K Lannon A Lath G Latino I Lazzizzera C Lecci T LeCompte J Lee S W Lee R Lefèvre N Leonardo S Leone S Levy J D Lewis K Li C Lin C S Lin M Lindgren E Lipeles T M Liss A Lister D O Litvintsev T Liu Y Liu N S Lockyer A Loginov M Loreti P Loverre R-S Lu D Lucchesi P Lujan P Lukens G Lungu L Lyons J Lys R Lysak E Lytken D MacQueen R Madrak K Maeshima P Maksimovic G Manca F Margaroli R Marginean C Marino A Martin M Martin V Martin M Martínez T Maruyama H Matsunaga M Mattson P Mazzanti K S McFarland D McGivern P M McIntyre P McNamara R McNulty A Mehta S Menzemer A Menzione P Merkel C Mesropian A Messina T Miao N Miladinovic J Miles L Miller R Miller J S Miller C Mills R Miquel S Miscetti G Mitselmakher A Miyamoto N Moggi B Mohr R Moore M Morello P A Movilla Fernandez J Muelmenstaedt A Mukherjee M Mulhearn T Muller R Mumford A Munar P Murat J Nachtman S Nahn I Nakano A Napier R Napora D Naumov V Necula J Nielsen T Nelson C Neu M S Neubauer T Nigmanov L Nodulman O Norniella T Ogawa S H Oh Y D Oh T Ohsugi T Okusawa R Oldeman R Orava W Orejudos K Osterberg C Pagliarone E Palencia R Paoletti V Papadimitriou A A Paramonov S Pashapour J Patrick G Pauletta M Paulini C Paus D Pellett A Penzo T J Phillips G Piacentino J Piedra K T Pitts C Plager L Pondrom G Pope X Portell O Poukhov N Pounder F Prakoshyn A Pronko J Proudfoot F Ptohos G Punzi J Rademacker M A Rahaman A Rakitine S Rappoccio F Ratnikov H Ray B Reisert V Rekovic P Renton M Rescigno F Rimondi K Rinnert L Ristori W J Robertson A Robson T Rodrigo S Rolli R Roser R Rossin C Rott J Russ V Rusu A Ruiz D Ryan H Saarikko S Sabik A Safonov R St Denis W K Sakumoto G Salamanna D Saltzberg C Sanchez L Santi S Sarkar K Sato P Savard A Savoy-Navarro P Schlabach E E Schmidt M P Schmidt M Schmitt T Schwarz L Scodellaro A L Scott A Scribano F Scuri A Sedov S Seidel Y Seiya A Semenov F Semeria L Sexton-Kennedy I Sfiligoi M D Shapiro T Shears P F Shepard D Sherman M Shimojima M Shochet Y Shon I Shreyber A Sidoti A Sill P Sinervo A Sisakyan J Sjolin A Skiba A J Slaughter K Sliwa

We measure the masses of b hadrons in exclusively reconstructed final states containing a J/psi --> mu-mu+ decay using 220 pb(-1) of data collected by the CDF II experiment. We find: m(B+) = 5279.10 +/- 0.41(stat.) +/- 0.36(sys.) MeV/c2, m(B0) = 5279.63 +/- 0.53(stat.) +/- 0.33(sys.) MeV/c2, m(B(s)0) = 5366.01 +/- 0.73(stat.) +/- 0.33(sys.) MeV/c2, m(lambda(b)0) = 5619.7 +/- 1.2(stat.) +/- 1.2(...

2008
A. D. Hardman R. M. Harris

The lifetime of the B0 s meson is measured using the semileptonic decay B0 s → D s l+νX. The data sample consists of about 110 pb−1 of pp̄ collisions at √ s = 1.8 TeV collected by the CDF detector at Fermilab. Four different D s decay modes are reconstructed resulting in approximately 600 D s l+ signal events. The B0 s meson lifetime is determined to be τ(B0 s ) = (1.36 ± 0.09 +0.06 −0.05) ps, w...

1998
A. D. Hardman R. M. Harris

The lifetime of the B0 s meson is measured using the semileptonic decay B0 s → D s l+νX. The data sample consists of about 110 pb−1 of pp̄ collisions at √ s = 1.8 TeV collected by the CDF detector at Fermilab. Four different D s decay modes are reconstructed resulting in approximately 600 D s l+ signal events. The B0 s meson lifetime is determined to be τ(B0 s ) = (1.36 ± 0.09 +0.06 −0.05) ps, w...

احتشامی, سید محمد رضا , زواره, محسن , پورابراهیمی, محیل ,

In order to investigate the effect of Pseudomonas fluorescence strain 93 bacteria and Glomus esculentum fungus on quantitative and qualitative yield of two forage corn cultivars, an RCBD based factorial field experiment with three replications was conducted at the Agricultural Research Station of the University of Guilan in 2008. Treatments were considered as phosphorus chemical fertilizer, se...

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