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  • 1
    Online Resource
    Online Resource
    Saint Louis :Elsevier Science & Technology,
    Keywords: Lattice field theory--Congresses. ; Electronic books.
    Type of Medium: Online Resource
    Pages: 1 online resource (699 pages)
    Edition: 1st ed.
    ISBN: 9781483278056
    DDC: 530.14
    Language: English
    Note: Front Cover -- Lattice 91 -- Copyright Page -- PREFACE -- Table of Contents -- Part 1: Plenary Talks -- Section 1.1: Reviews -- CHAPTER 1. THE QCD SPECTRUM AND PHASE DIAGRAM ON THE LATTICE - 1991 -- Introduction -- The QCD spectrum on the lattice -- Phase structure of QCD -- Acknowledgments -- References -- CHAPTER 2. QCD AT FINITE DENSITY -- 1. Formulation -- 2. The Quenched Approximation [3] -- 3. Monte-Carlo simulations with dynamical fermions -- 4. The Propagator Matrix -- 5. Monte-Carlo simulations measuring the canonical partition functions in SU (3) -- Acknowledgements -- References -- CHAPTER 3. WEAK MATRIX ELEMENTS -- Introduction -- The kaon B-parameter -- Divergent Operators -- Conclusion -- Acknowledgements -- References -- CHAPTER 4. SIMULATING HEAVY QUARKS -- 1. Introduction -- 2. Why Study Quarkonium? -- 3. Dirac Quarks-Wilson's Action -- 4. Nonrelativistic Quarks-NRQCD -- 5. Static Quarks -- 6. Lattice Perturbation Theory -- 7. Applications -- 8. Summary and Conclusions -- Acknowledgements -- References -- CHAPTER 5. HIGGS- AND YUKAWA-THEORIES ON THE LATTICE -- 1. INTRODUCTION -- 2. SCALAR HIGGS MODELS -- 3. SCALAR-FERMION YUKAWA-MODELS -- 4. SUMMARY AND CONCLUSIONS -- References -- CHAPTER 6. SPHALERON INDUCED BARYON NUMBER NON-CONSERVATION -- 1. Introduction -- 2. Rate of sphaleron transitions at high temperatures -- 3. Real time lattice simulations of sphaleron transitions -- 4. Electroweak baryogenesis -- 5. Conclusion -- References -- CHAPTER 7. QUANTUM GRAVITY AND RANDOM SURFACES -- 1. Introduction -- 2. Two-dimensional quantum gravity -- 3. Random surfaces -- 4. Quantum gravity in d > -- 2 -- 5. Conclusion -- Acknowledgements -- References -- CHAPTER 8. RECENT ANALYTIC PROGRESS ON FINITE SIZE EFFECTS -- 1. INTRODUCTION -- 2. SIGNATURES OF RESONANCES IN FINITE VOLUME -- 3. CHIRAL PERTURBATION THEORY. , 4. THE THERMODYNAMIC BETHE ANSATZ -- 5. DETERMINATION OF THE RUNNING COUPLING -- 6. FIRST ORDER TRANSITIONS -- References -- CHAPTER 9. PARALLEL QCD MACHINES -- 1. INTRODUCTION -- 2. BACKGROUND -- 3. FIRST GENERATION -- 4. SECOND GENERATION -- 5. COMMERCIAL MACHINES -- 6. NEW PROJECTS -- 7. CONCLUSIONS -- References -- CHAPTER 10. MULTIGRID METHODS IN LATTICE FIELD COMPUTATIONS -- 1. Elementary Acquaintance with Multigrid -- 2. Introduction -- 3. Multigrid PDE Solvers -- 4. Multigrid Dirac Solver -- 5. Multiscale Statistical Simulations -- 6. Other Relevant Multilevel Techniques -- Acknowledgements -- References -- CHAPTER 11. THEORY AND NUMERICAL SIMULATION OF COMPUTATIONALLY DIFFICULT SYSTEMS -- 1. Introduction -- 2. NP Completeness -- 3. The Energy Landscape -- 4. The Pure States -- 5. Some Soluble Models -- 6. An Open Case: Three Dimensional Spin Glasses -- 7. Pinned Manifolds -- 8. Random Self-Interacting Heteropolymers -- 9. Conclusions -- References -- Section 1.2: Topical Talks -- CHAPTER 12. TOWARDS THE CONTINUUM LIMIT OF STAGGERED WEAK MATRIX ELEMENTS -- 1. INTRODUCTION -- 2. FLAVOR SYMMETRY BREAKING -- 3. SCALING OF QUENCHED BK -- 4. IMPROVED OPERATORS -- ACKNOWLEDGEMENTS -- References -- CHAPTER 13. LATTICE APPROACH TO SEMI-LEPTONIC DECAYS OF CHARM MESONS -- 1. Introduction -- 2. The Status at LAT'90 -- 3. Experiments and Phenomenology -- 4. Lattice Methodology and Differences in Implementation -- 5. Results -- 6. Remarks on the Pole-Dominance Model and on the End-point Region -- 7. Conclusions and Summary -- Acknowledgements -- References -- CHAPTER 14. FIRST RESULTS FROM THE UKQCD COLLABORATION -- 1. Introduction -- 2. Details of Simulation -- 3. Static Q - Q Potentials -- 4. The Hadron Spectrum -- Conclusions -- References -- CHAPTER 15. RECENT RESULTS FROM THE 256-NODE COLUMBIA MACHINE -- 1. Introduction -- 2. Nt = 2 Hadron Masses. , References -- CHAPTER 16. INVESTIGATION OF THE FERMION SPECTRUM AT STRONG WILSON-YUKAWA COUPLING IN THE SYMMETRIC PHASE -- 1. INTRODUCTION -- 2. THE FERMION SPECTRUM IN THE PMS PHASE -- 3. THE NEUTRAL FERMION SECTOR -- 4. THE CHARGED FERMION SECTOR -- 5. FINAL REMARKS -- References -- CHAPTER 17. ON LATTICE CHIRAL GAUGE THEORIES -- References -- CHAPTER 18. THE GENERALIZED NAMBU-JONA-LASINIO MECHANISM AND THE STANDARD MODEL -- 1. Introduction -- 2. The Nambu-Jona-Lasinio Model -- 3. Equivalent Higgs-Yukawa Model -- 4. Equivalence Proof in the 1/N Expansion -- 5. Hill's Toy Model and the NJL Condensate -- 6. Conclusions -- Acknowledgements -- References -- CHAPTER 19. VORTEX SCATTERING IN THE ABELIAN HIGGS MODEL -- References -- CHAPTER 20. THE EXACT MASS GAP IN D=2 ASYMPTOTICALLY FREE FIELD THEORIES AND RELATED EXPERIMENTAL RESULTS -- 1. Introduction and Summary -- 2. An Application: The Magnetic Correlation Length of La2CuO4 Compounds at Low Temperatures -- 3. General Steps and Assumptions Leading to the Mass Gap Predictions -- Acknowledgements -- References -- CHAPTER 21. ON SELF ORGANIZED CRITICALITY -- Acknowledgement -- References -- Part 2: Parallel Sessions -- Section 2.1 QCD -- 2.1.1 QCD Spectroscopy -- CHAPTER 22. QCD HADRON SPECTROSCOPY WITH STAGGERED DYNAMICAL QUARKS AT -- Acknowledgements -- References -- CHAPTER 23. FINITE-SIZE EFFECTS AND Tc FOR ß = 5.445 WITH TWO STAGGERED FLAVORS -- References -- CHAPTER 24. FULL QCD HADRON SPECTROSCOPY AT ß = 5.7 -- 1. INTRODUCTION -- 2. FINITE-SIZE EFFECT -- 3. PHYSICAL SCALE OF THE LATTICE -- 4. fπ AND BK IN FULL QCD -- References -- CHAPTER 25. HADRON SPECTRUM AND INTERQUARK FORCES: RESULTS FROM THE MTC COLLABORATION -- 1. HADRON SPECTRUM -- 2. CHIRAL SECTOR -- 3. HEAVY QUARK POTENTIAL -- References -- CHAPTER 26. SIMULATIONS OF 2-FLAVOR QCD ON A 324 LATTICE AT ß = 5.7 -- 1. INTRODUCTION. , 2. Tests of 163 x 32 Simulation -- 3. Currently running 324 simulations -- References -- CHAPTER 27. DYNAMICAL QUARK EFFECTS ON GLUEBALLS AND TOPOLOGY IN LATTICE QCD -- 1. INTRODUCTION -- 2. GLUEBALL MASS SPECTRUM -- 3. TOPOLOGICAL SUSCEPTIBILITY -- References -- CHAPTER 28. THE QUENCHED MASS SPECTRUM IN LATTICE QCD -- 1. Introduction -- 2. The Hadron Masses and the Chiral Limit -- 3. The Mass Splittings -- 4. The Physical Mass Values and the Scaling Behaviour -- 5. Decay Constants and the Nucleon σ Term -- References -- CHAPTER 29. QUENCHED HADRON SPECTRUM ON A 243 x 54 LATTICE -- References -- CHAPTER 30. FLAVOR SYMMETRY OF HADRON MASSES WITH STAGGERED FERMIONS -- 1. Introduction -- 2. Wall Source Technique -- 3. Result -- 4. Summary -- References -- CHAPTER 31. VOLUME DEPENDENCE OF THE VALENCE WILSON FERMION MASS SPECTRUM -- References -- CHAPTER 32. QCD SPECTROSCOPY AND PHENOMENOLOGY WITH IMPROVED ACTIONS -- 1. Introduction -- 2. Phenomenology: Clover vs. Wilson -- 3. Spectroscopy with the Hamber-Wu Action -- References -- CHAPTER 33. HADRON SPECTROSCOPY ON A 323 x 48 LATTICE -- 1. Introduction -- 2. Measurement of Hadron Propagators -- Acknowledgment -- References -- 2.1.2 Finite-Temperature QCD -- CHAPTER 34. THE CHIRAL PHASE TRANSITION IN QCD: CRITICAL EXPONENTS AND THEIR FLAVOUR DEPENDENCE -- 1. UNIVERSALITY AND CHIRAL SYMMETRY ON THE LATTICE -- 2. ONE SPECIES OF STAGGERED FERMIONS -- 3. SEVERAL SPECIES OF STAGGERED FERMIONS -- References -- CHAPTER 35. DECONFINING TRANSITION OF SU(S) GAUGE THEORY ON NT = 6 LATTICES -- References -- CHAPTER 36. QCD THERMODYNAMICS WITH TWO FLAVORS OF QUARKS[1] -- References -- CHAPTER 37. THERMODYNAMICS OF LATTICE QCD WITH 2 LIGHT DYNAMICAL (STAGGERED) QUARK FLAVOURS ON A 163 x 8 LATTICE -- References -- CHAPTER 38. QUARK CONFINEMENT AND NUMBER OF FLAVORS -- References. , CHAPTER 39. QCD PHASE STRUCTURE WITH 8 LIGHT QUARK FLAVORS -- 1. Introduction -- 2. Strong First Order Transition and ßc -- 4. Chiral Properties of the Phases -- 5. Conclusion -- References -- CHAPTER 40. THE BUBBLE FREE ENERGY IN THE QCD PHASE TRANSITION -- References -- CHAPTER 41. FULL QCD AND QED AT FINITE TEMPERATURE AND CHEMICAL POTENTIAL -- 1. Full QCD on anisotropic lattices -- 2. Full QED with finite chemical potential -- References -- CHAPTER 42. SCREENING IN HOT QCD -- ACKNOWLEDGEMENTS -- References -- CHAPTER 43. COMPLEX ZEROS OF THE PARTITION FUNCTION FOR LATTICE GAUGE THEORIES -- 1. Introduction -- 2. Z[m,ß] as a Polynomial in the Mass -- 3. Results -- References -- CHAPTER 44. THE DEBYE SCREENING IN THE QUARK-GLUON PLASMA -- References -- 2.1.3 Weak Matrix Elements -- CHAPTER 45. MATRIX ELEMENTS WITH WILSON FERMIONS -- 1. INTRODUCTION -- 2. SURPRISES IN HADRON SPECTRUM -- 3. MESON DECAY CONSTANTS -- 4. CHIRAL PARAMETERS mq and ψψ -- 5. KAON B PARAMETER -- ACKNOWLEDGEMENTS -- References -- CHAPTER 46. IMPROVED LATTICE QCD -- 1. Introduction -- 2. Next-to-nearest-neighbor improved action -- 3. Nearest-neighbor improved action -- Acknowledgements -- References -- CHAPTER 47. HEAVY FLAVOR MESON DECAY CONSTANTS WITH WILSON FERMIONS AT ß = 6.4 -- References -- CHAPTER 48. FLAVOR CHANGING NEUTRAL CURRENT TRANSITIONS ON THE LATTICE FOR HEAVY-LIGHT SYSTEMS -- References -- CHAPTER 49. SCALAR AND AXIAL MATRIX ELEMENTS OF THE NUCLEON: SEA QUARK CONTENT -- ACKNOWLEDGEMENTS -- References -- CHAPTER 50. QUARK LOOP CALCULATIONS -- References -- CHAPTER 51. THE QUARK FRACTION OF THE PROTON SPIN -- 1. INTRODUCTION -- 2. THEORETICAL PRELIMINARIES -- 3. LATTICE ANALYSIS -- 4. RESULTS -- 5. CONCLUSIONS -- ACKNOWLEDGEMENTS -- References -- CHAPTER 52. CHIRAL PERTURBATION THEORY FOR THE QUENCHED APPROXIMATION -- References. , CHAPTER 53. FROM THE LATTICE WORLD TO THE REAL WORLD.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 5057-5059 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Nanometer-scale mounds were fabricated by applying voltage pulses between a substrate and an atomic force microscope cantilever coated with magnetic material. Mounds were formed on both insulator and conducting substrates. Magnetic force microscopy (MFM) observations of the fabricated mounds were performed, and the contrast was turned over by reversing the magnetization of the tip, which is convincing proof that the mounds are magnetic. The MFM images also suggest that the mounds are perpendicularly magnetized. These results demonstrate that scanning probe microscope based nanofabrication is a promising method to fabricate nanoscale magnetic dots on any kind of substrates. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 772-779 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: To advance new soft magnetic materials of an FeGaSi alloy into the commercial world, improvements on various properties were designed by introducing additive elements without sacrificing its high saturation magnetic induction. The detailed studies on the diversified properties, such as saturation magnetic induction, film internal stress, wear resistivity, and so on, were performed. High-frequency permeability of the laminated structure film was also investigated. As a result, the Ru-added FeRuGaSi alloy films, whose typical compositions are Fe72Ru4Ga7Si17 and Fe68Ru8Ga7Si17 (at. %), prove to be excellent soft magnetic materials especially appropriate for the magnetic recording/playback head core use.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 2983-2992 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetic and other properties of Co-base amorphous alloy films prepared by sputtering are investigated. A detailed magnetic phase diagram with saturation magnetic flux density, crystallization temperature, and zero-magnetostrictive line on Co-Ta-Zr amorphous alloys were obtained, and the technical knowhow to make a film with well-reproducible characteristics by widely changing the sputtering conditions was related with these physical properties. Especially on alloy sputtering, a phenomenological model for elucidating a composition difference between film and target is presented. After these studies, the film characteristics of Bs=12 kG, Tx=450 °C, ||λs||〈10−8, Hc〈10 mOe, and permeabilities of μ(1 MHz)=7000, μ(100 MHz)=2000 for the single film of 2 μm in thickness and of μ(1 MHz)=4000, μ(100 MHz)=800 for the insulator-sandwiched multilayered film of 10 μm are obtained, and these well-balanced values enable us to apply the materials for high-frequency recording head.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 81 (1997), S. 5021-5023 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Coupling of soft magnetic films to antiferromagnetic substrates was studied by spin-polarized secondary electron microscopy. Permalloy (Ni80Fe20 alloy) films were deposited on antiferromagnetic NiO(111) single-crystal substrates. A domain structure consisting of fine grains (∼50 μm) was characteristic of the NiFe film deposited without applying magnetic field. The domain image and its response to applied field suggested existance of local easy axis and local unidirectional anisotropy. When macroscopic unidirectional anisotropy was introduced to the NiFe film by depositing under an applied dc magnetic field, many of the fine grains disappeared and the film showed large domains (∼1 mm). In the large domains, small elongated reversed domains (∼20 μm×60 μm) aligned parallel to each other implying local easy axis of magnetization. The type of domain behavior described above was not observed in a NiFe film on MgO(111) substrate that had the same crystal structure as NiO but no magnetic ordering. An x-ray analysis revealed that the local easy axes observed in NiFe/NiO specimens coincided with the [112¯] of the NiO crystal lying in the (111) substrate plane, which supported coupling of the NiFe film with the single-crystal substrate. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 6582-6584 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The coercive forces and anisotropy fields of Fe-Ru-Ga-Si films deposited on 30° tilted substrates were measured for varying chemical compositions and crystal orientations. The minimum coercivity and minimum in-plane magnetic anisotropy were observed at an iron-rich composition corresponding to a substantial magnitude of anisotropy constant: K1=6×103 (J/m3). From an orientation analysis of the crystal aggregate, this optimization with the large K1 was understood to be a result of the cancellation of the shape anisotropy by the crystalline anisotropy.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 3514-3519 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Extensive study was made on Fe-base crystalline alloys in search for new soft magnetic materials with high saturation magnetization by means of sputtering technique. It revealed that newly found FeGaSi and FeAlGe alloy systems possessed excellent soft magnetic properties with remarkably higher saturation magnetization. These new alloy films, annealed in vacuum at 500 °C for 1 h, show the magnetic properties of Bs=13 and 15 kG, Hc=0.09 and 0.20 Oe, and μ1 MHz=2000 and 1800 for the FeGaSi and FeAlGe alloy films of 2 μm in thickness, respectively. These values are superior to those of FeAlSi (sendust) alloy which is a typical soft magnetic material with high saturation magnetization. Results of the Co-added systems of FeCoGaSi and FeCoAlGe alloys are also presented. Discussions are given on various systems of Fe base crystalline alloy films studied, which are classified into four types of groups with respect to magnetic softness.
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  • 8
    ISSN: 1365-3083
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Medicine
    Notes: To clarify the significance of basic fetoprotein (BFP) in lymphocytes, we investigated whether BFP is produced in lymphocytes during blastic transformation. Peripheral blood lymphocytes obtained from 14 adults were cultured under the stimulation of lectins. The concentration of BFP in the culture medium (extracellular BFP) was estimated serially. The incorporation of [6-3 H] thymidine was assayed simultaneously. The intracellular BFP was measured by dual flow cytometry for DNA and BFP. A lymph node was studies immunohistochemically. Serum BFP was measured in four cases of lumphocytic leukaemia. In two cases, dual staining was performed. The intracellular BFP of the mitogen-stimulated lymphocytes was increased within 24 h. The extracellular BFP was increased exponentially from 72 h. The extracellular BFP at 96 h did not correlate with the [3H]-thymidine incorporation. The intracellular BFP increase began in G1 phase. Immunostaining showed that the B cells also produced BFP. Theserum BFP level in leukaemia was high in 1 of 4 cases and the leukaemic cells in two cases showed high intracellular BFP content. These observations indicate that BFP is produced in activated human lymphocytes and in lymphocytic leukaemic cells. The production of BFP during blastic transformation will be a useful new in vitro model for studying the biological role of BFP, and BFP labelling may offer some new possibilities for study of lymphocytes.
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  • 9
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Science Ltd
    Journal of neuroendocrinology 16 (2004), S. 0 
    ISSN: 1365-2826
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Medicine
    Notes: Tuberoinfundibular corticotropin-releasing hormone (CRH) neurones are the principal regulators of the hypothalamic-pituitary-adrenal (HPA)-axis. Vasopressin is primarily a neurohypophysial hormone, produced in magnocellular neurones of the hypothalamic paraventricular and supraoptic nuclei, but parvocellular CRH neurones also coexpress vasopressin, which acts as a second ‘releasing factor’ for adrenocorticotropic hormone along with CRH. All stress inputs converge on these hypothalamic neuroendocrine neurones, and the input signals are integrated to determine the output secretion of CRH and vasopressin. Aminergic, cholinergic, GABAergic, glutamatergic and a number of peptidergic inputs have all been implicated in the regulation of CRH/vasopressin neurones. Glucocorticoids inhibit the HPA-axis activity by negative feedback. Interleukin-1 stimulates CRH and vasopressin gene expression, and is implicated in immune-neuroendocrine regulation. cAMP-response element-binding protein phosphorylation may mediate transcriptional activation of both CRH and vasopressin genes, but the roles of AP-1 and other transcription factors remain controversial. Expression profiles of the CRH and vasopressin genes are not uniform after stress exposure, and the vasopressin gene appears to be more sensitive to glucocorticoid suppression.
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  • 10
    ISSN: 1365-3040
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Biology
    Notes: The GA-signal transduction pathways downstream to the Gα protein in rice seedling root were investigated using in-gel kinase assay and in vitro protein phosphorylation techniques with a Gα protein defective mutant, d1. A 50-kDa protein kinase was detected downstream to Gα protein in the membrane fraction of rice seedling roots using an in-gel kinase assay with histone III-S as a substrate. The activity of a 50-kDa protein kinase increased in the wild-type rice by gibberellin (GA3) treatment, but did not change in the d1 mutant. This protein kinase activity was inhibited by the Ca2+ chelator ethyleneglycol-bis-(beta-aminoethylether)-N,N,N 1,N 1-tetraacetic acid (EGTA), protein kinase inhibitors, staurosporine and H7, and calmodulin antagonist, trifluoperazine, suggesting that the 50-kDa protein kinase is a putative plant Ca2+-dependent protein kinase (CDPK). The activity of the 50-kDa putative CDPK reached its highest level at 3 h after GA3 treatment and then gradually declined with time. In order to identify the endogenous substrate for 50-kDa putative CDPK, two-dimensional polyacrylamide gel electrophoresis followed by in vitro protein phosphorylation was carried out. The phosphorylation activity of an endogenous protein PP30, identified as an unknown protein having molecular weight 30 kDa and isoelectric point 5.8 was increased in the wild-type rice by GA3 treatment, compared with the d1 mutant. The addition of GA3 treated membrane fraction, which predominantly represent a 50-kDa putative CDPK further increased the phosphorylation of PP30. Almost similar to GA3 treatment, phosphorylation activity of PP30 was also increased by the treatment with cholera toxin in the wild-type rice but not in d1 mutant. These results suggest that the 50-kDa putative CDPK and an unknown protein, PP30 promoted by GA3 treatment are G-protein mediated in rice seedling roots.
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