1 Decay Scheme. 2 Nuclear Data. 236m. 2.1 Electron Capture Transitions. 2.2 β Transitions
|
|
|
- Ê Αλεξάνδρου
- 5 χρόνια πριν
- Προβολές:
Transcript
1 1 Decay Scheme Np- (isomer state of Np-236, J=1, E1 =60 ) decays 53(1) % by electron capture to U-236 and 47(1) % by beta minus emission to Pu-236. Le neptunium 236 isomère se désintègre par capture électronique (53%) vers l uranium 236 et par transition bêta moins vers le plutonium Nuclear Data T 1/2 ( Np ) : 22,5 (4) h T 1/2 ( 236 U ) : 23,43 (6) 10 6 a T 1/2 ( 236 Pu ) : 2,87 (1) a Q ( Np ) : 537 (8) Q ( Np ) : 993 (13) 2.1 Electron Capture Transitions Probability Nature lg ft P K P L P M 100 ɛ 0,4 306 (13) 1,64 (9) 1st forbidden 7,3 0,621 (10) 0,274 (7) 0,105 (3) ɛ 0,1 948 (13) 8,3 (30) allowed 7,8 0,751 (1) 0,184 (1) 0,0652 (1) ɛ 0,0 993 (13) 43,1 (32) allowed 7,1 0,753 (1) 0,182 (1) 0,0646 (1) 2.2 β Transitions Probability Nature lg f t 100 β0,1 492 (8) 11 (4) allowed 7,2 β0,0 537 (8) 36 (4) allowed 6,8 KRI /Chechev V.P. and Kuzmenko N.K. 1 10/07/ /1/2012
2 2.3 Gamma Transitions and Internal Conversion Coefficients P γce Multipolarity α K α L α M α T 100 γ 1,0(Pu) 44,63 (10) 11,2 (37) E2 540 (11) 151 (3) 743 (15) γ 1,0(U) 45,242 (3) 9,6 (30) E2 429 (9) 118,6 (24) 589 (12) γ 2,1(U) 104,234 (15) 0,0143 (17) E2 8,00 (16) 2,22 (5) 11,0 (2) γ 4,2(U) 538,11 (10) 0,0143 (17) E3 0,0622 (13) 0,0587 (12) 0,0160 (4) 0,143 (3) γ 4,1(U) 642,35 (9) 1,24 (8) E1(M2E3) 0,112 (10) 0,031 (3) 0,0080 (8) 0,15 (2) γ 4,0(U) 687,60 (5) 0,383 (28) E1 0,219 (12) 0,068 (6) 0,018 (2) 0,31 (2) 3 Atomic Data 3.1 U ω K : 0,970 (4) ω L : 0,500 (19) ω M : 0,050 (5) n KL : 0,794 (5) X Radiations Relative probability K Kα 2 94,666 62,47 Kα 1 98, Kβ 3 110,421 } Kβ 1 111,298 } Kβ 5 111,964 } 36,08 Kβ 2 114,407 } Kβ 4 115,012 } 12,34 KO 2,3 115,377 } L Ll 11,618 Lα 13,438 13,614 Lη 15,399 Lβ 15,726 18,206 Lγ 19,507 20,714 KRI /Chechev V.P. and Kuzmenko N.K. 2 10/07/ /1/2012
3 3.1.2 Auger Electrons Relative probability Auger K KLL 71,776 80, KLX 88,153 98,429 59,6 KXY 104,51 115,59 8,88 Auger L 6,4 21,6 3.2 Pu ω K : 0,971 (4) ω L : 0,521 (20) ω M : 0,555 (5) n KL : 0,790 (5) 4 Electron Emissions Electrons per 100 disint. e AL (U) 6,4-21,6 21,7 (15) e AK (U) 1,03 (17) KLL 71,776-80,954 } KLX 88,153-98,429 } KXY 104,51-115,59 } e AL (Pu) 6,6-23,0 3,8 (14) ec 1,0 L (Pu) 21,53-26,57 8 (3) ec 1,0 L (U) 23,484-28,074 6,9 (22) ec 1,0 M (Pu) 38,70-40,86 2,2 (8) ec 1,0 M (U) 39,694-41,690 1,9 (6) ec 4,1 K (U) 526,75 (9) 0,121 (13) ec 4,0 K (U) 572,00 (5) 0,064 (6) β0,1 max: 492 (8) 11 (4) β0,1 avg: 143 (3) β0,0 max: 537 (8) 36 (4) β0,0 avg: 158 (3) KRI /Chechev V.P. and Kuzmenko N.K. 3 10/07/ /1/2012
4 5 Photon Emissions 5.1 X-Ray Emissions Photons per 100 disint. XL (U) 11,618 20,714 21,3 (18) XKα 2 (U) 94,666 9,9 (10) } Kα XKα 1 (U) 98,44 15,8 (15) } XKβ 3 (U) 110,421 } XKβ 1 (U) 111,298 } 5,7 (6) K β 1 XKβ 5 (U) 111,964 } XKβ 2 (U) 114,407 } XKβ 4 (U) 115,012 } 1,95 (15) K β 2 XKO 2,3 (U) 115,377 } XL (Pu) 12,124 21,984 4,2 (16) 5.2 Gamma Emissions Photons per 100 disint. γ 1,0 (Pu) 44,63 (10) 0,015 (5) γ 1,0 (U) 45,242 (3) 0,016 (5) γ 2,1 (U) 104,234 (6) 0,00119 (14) γ ± 511 γ 4,2 (U) 538,11 (10) 0,0125 (15) γ 4,1 (U) 642,35 (9) 1,08 (6) γ 4,0 (U) 687,60 (5) 0,292 (21) 6 Main Production Modes U 235(d,n)Np U 235(α,p,2n)Np 7 References - R.A.James, A.E.Florin, H.H.Hopkins, Jr., A.Ghiorso. NNES 14B (1949) 1604 (Half-life) - P.R. Gray. Phys.Rev. 101 (1956) 1306 (Relative probability of K-electron capture in the decay of -Np) - J.E. Gindler, R.K. Sjoblom. J. Inorg. Nucl. Chem. 12 (1959) 8 (Probabilities of beta transitions) - J.A. Bearden. Rev. Mod. Phys. 39 (1967) 78 (X-ray energies) KRI /Chechev V.P. and Kuzmenko N.K. 4 10/07/ /1/2012
5 - C.M. Lederer, J.M. Jaklevic, S.G. Prussin. Nucl. Phys. A135 (1969) 36 (Relative intensities of gamma rays) - R. Gunnink, R.J. Morrow. In: UCRL (1971) (Emission probabilities of gamma-rays in the decay of 240Pu) - O. Dragoun, Z. Plajner, F. Schmutzler. NDT A9 (1971) 119 (am / al and ano / am) - B.S. Dzhelepov, L.N. Zyryanova, Yu.P. Suslov. Beta-processes, 1972, Nauka, Leningrad (1972) (Fractional probabilities in L-electron capture) - T. Dragnev, K. Scharf. Intern. J. Appl. Radiat. Isotop. 26 (1975) 125 (Gamma ray emission probabilities in the decay of 240Pu) - H. Ottmar, P. Matussek, I. Piper. Proc Int Symp Neutron Capture Gamma Ray Spectr. and Related Top., 2nd, Petten, Netherlands1974, K. Abrahams e.a., Eds, Reactor Centrum Nederland (1975) 658 (Emission probabilities of gamma-rays in the decay of 240Pu) - R. Gunnink, J.E. Evans, A.L. Prindle. UCRL (1976) (Emission probabilities of gamma-rays in the decay of 240Pu) - W.L. Posthunus, K.E.G. Löbner, I. Piper e.a.. Z. Phys. A181 (1977) 717 (ICC measurements) - F.P. Larkins. Atomic Data and Nuclear Data Tables. 20 (1977) 313 (Auger electron energies) - E.A.Gromova, S.S.Kovalenko, Yu.A.Nemilov, Yu.A.Selitsky, A.V.Stepanov, A.M.Fridkin, V.B.Funshtein, V.A.Yakovlev, G.V.Valsky, G.A.Petrov. Sov.At. 56 (1984) 230 (Half-life) - F. Lagoutine, N. Coursol, J. Legrand. ISBN (LMRI, ). (1987) ( of Auger electrons) - M.R.Schmorak. Nucl.Data Sheets 63 (1991) 139 (Decay scheme, gamma ray multipolarities) - E. Schönfeld, H. Janssen. Nucl. Instrum. Methods Phys. Res. A369 (1996) 527 (Atomic data) - R.B. Firestone. Table of Isotopes, Eighth Edition, Vol.II: A= , V.S. Shirley, C.M. Baglin, S.Y.F. Chu, and J. Zipkin, 1996, 1998, 1999 (1996) (Decay scheme, LX ray energies, multipolarities) - E. Schonfeld, G. Rodloff. PTB , Braunschweig, February 1999 (1999) (KX-ray energies and relative emission probabilities) - G. Audi, A.H. Wapstra, C. Thibault. Nucl. Phys. A729 (2003) 337 (Q values) - M.-M. Bé, V. Chiste, C. Dulieu, E. Browne, V. Chechev, N. Kuzmenko, R. Helmer, A. Nichols, E. Shonfeld, R. Dersch.. Table of Radionuclides, Vol.2. A = 151 to Pu. Bureau International des Poids et Mesures, 2004 (2004) (Recommended Data by the Decay Data Evaluation Project working group) KRI /Chechev V.P. and Kuzmenko N.K. 5 10/07/ /1/2012
6 LNE-LNHB/CEA - Table de Radionucléides Np 236 m γ Emission intensities per 100 disintegrations m ε β - Np ; 0 22,5 (4) h 3,8 ns ,01 1,08 0,29-1 ; 687,6 1 γ Emission intensities per 100 disintegrations 5 0,01 2 ; 44,63 58 ps 3 6 ; 309, ps ps 1 23,43 (6) x10^6 a 0 0, , U Q = 993 % = 53 4 ; 149,476 2 ; 45,242 0 ; Pu Q = 537 % = 47 0 ; 0 2,87 (1) a KRI / Chechev V.P. and Kuzmenko N.K. Scheme page : 1/1 10/07/ /07/2006
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Np decays 87,8 (6) % by electron capture to U, 12,0 (6) % by beta minus emission to Pu, a possible alpha emission of 0,16 (6)% to Pa232 has not been observed. Le neptunium se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Cf- disintegrates by alpha emissions mainly to the Cm-248 ground state level, and by spontaneous fission for 3,086(8) %. The average number of neutrons emitted by spontaneous fission is:
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β Transitions
1 Decay Scheme Le césium se désintègre essentiellement par émission bêta moins vers des niveaux excités du baryum. Cs- desintegrates mainly by beta minus emissions to excited levels in Ba-. 2 Nuclear Data
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Bi- disintegrates 97.91(3) % by beta minus emission to the levels in Po- and 2.09(3) % through alpha decay to Tl-209. Le bismuth se désintègre principalement par émissions bêta vers le polonium
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
1 Decay Scheme I- disintegrates by electron capture mainly via the 159 level of Te- (97%). L iode se désintègre par capture électronique principalement vers le niveau excité de 159 du tellure, avec une
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Pb ground state (J π = 9/2 + ) decays by 100 % beta minus to Bi. The strongest branch (91.28 (12) %) decays directly to the ground state (J π = 9/2 ). Le plomb se désintègre par émissions
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pu- decays approximately 100 % by beta minus emission to the ground state of Am- and 0,00244 % by alpha emission to levels of U-237. The spontaneous fission decay branching is less than
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Bi- undergoes beta decay to Po- (64.07(7)%), and alpha decay to Tl-208 (35.93(7)%). 0.014(1)% of the beta branch undergoes prompt long-range alpha decay to Pb-208. Le bismuth se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme In- disintegrates by > 99.99% electron capture via the excited level of 416.6 in Cd- and by < 0.01% electron capture via the isomer level in Cd- (T 1/2 = 48.5 min) at 396.2. Transitions
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Sn- decays by electron capture mainly to the In-m isomer which has a half-life of 99 minutes. After a sufficient time, the ratio of the In-m (99 min) and Sn- activities remains constant
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pa is a member of the natural U235 decay chain. Pa disintegrates by alpha emission to various excited levels and the ground state of Ac227. Le protactinium se désintègre par émissions alpha
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme U- disintegrates by alpha emission mainly to the ground and 49- states in Th-232, and by 9,3 10 8 % spontaneous fission. L uranium se désintègre par émission alpha et par fission spontanée
1 Decay Scheme. 2 Nuclear Data. 2.1 β + Transitions. 2.2 Electron Capture Transitions
1 Decay Scheme Ni disintegrates by electron capture (56.6 %) and positron emission (43.4 %) to excited levels in Co. The transition to the ground state has not been observed. Le nickel se désintègre par
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Pb disintegrates by beta minus emission to excited levels and to the ground state level of Bi. Le plomb se désintègre par émission bêta moins vers des niveaux excités et le niveau fondamental
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Rh- disintegrates by beta minus emission to the ground state and excited levels of Pd-. Le rhodium se désintègre par émission bêta principalement vers le niveau fondamental et les niveaux
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Am decays by emission of alpha particles to Np239, with a minute branch of 3.8 (7) 10 9 % by spontaneous fission. L américium se désintègre par émission alpha vers le neptunium 239. Un faible
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Se disintegrates 100% by electron capture to excited levels and to the ground state of As. Le Se se désintègre à 100% par capture électronique vers des niveaux excités et le niveau fondamental
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Eu- disintegrates 100 % via beta minus disintegration to excited levels and to the ground state in Gd-. L europium se désintègre par émission bêta moins vers des niveaux excités et le niveau
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Co disintegrates by 100% electron capture to the excited levels of 706.42 (0.18%), and 136.47 (99.82%) in Fe. Le cobalt se désintègre à 100 % par capture électronique principalement vers
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Cm decays 1% by alpha transitions to Pu38 and by spontaneous fission with branching fraction of 6.36 (14) E6 %. Le curium se désintègre à 1% par transition alpha vers le plutonium 38 et
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Cm- decays 100% by alpha transitions to Pu-240 and by spontaneous fission with branching fraction of 1.36 (1) E-4 %. Le curium se désintègre par émission alpha et par fission spontanée dans
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Uranium decays primarily by alpha decay to excited states in Th-228. A small branching of exotic decay via Ne-24 emission and a smaller branching of spontaneous fission have been reported.
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Pb- disintegrates by electron capture to Tl- via excited levels. Le plomb se désintègre par capture électronique vers des niveaux excités du thallium. 2 Nuclear Data T 1/2 ( Pb ) : 51,929
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Nd- disintegrates by beta minus emission to excited levels of Pm-. If a transition to the ground state level exists, it is less than 0.15 %. Le néodyme se désintègre par émission bêta moins
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pu- decays 100% by alpha transitions to U-234. Most of the alpha decay populates the U-234 ground state (71.04 %) and the U-234 first excited level with energy of 43.50 (28.85 %). Branching
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
1 Decay Scheme - disintegrates 19.58 (11) % by beta plus emission and 8.2 (11) % by electron capture to Fe-. - emits gamma rays with energies up to 612 and the energies and emission probabilities for many
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β + Transitions
1 Decay Scheme Zr- (half-life of 78.42 h) undergoes 100% EC/positron decay (Q EC of 2832.8(28) kev) to various nuclear levels, including the metastable and ground states of Y-. Le zirconium se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
1 Decay Scheme Ba disintegrates by electron capture mainly to two Cs excited levels of 437 kev (85.4%) and of 383 kev (14.5%) with three very minor branches to the 160 kev, 81 kev excited levels and the
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Co decays 100% by electron capture to the excited levels of 706.42 kev (0.183%) and 136.47 kev (99.80%) in Fe. Le cobalt se désintègre par capture électronique vers des niveaux excités du
Th, Ra, Rn, Po, Pb, Bi, & Tl K x-rays. Rn Kα1. Rn Kα2. 93( 227 Th)/Rn Kβ3. Ra Kα2. Po Kα2 /Bi K α1 79( 227 Th)/Po Kα1. Ra Kα1 /Bi K β1.
Page -1-10 8 10 7 10 6 10 5 10 4 334 ( Th) Counts/Channel 10 3 10 2 10 1 49 ( Th)/ 50 ( Th)/ 50 ( Fr) 0 100 200 300 400 500 600 700 800 900 1000 1000 1100 1200 1300 1400 1500 1600 1700 1800 1900 2000 Channel
5.7. TABLE OF PHYSICAL CHARACTERISTICS OF RADIONUCLIDES MENTIONED IN THE EUROPEAN PHARMACOPOEIA
01/2008:50700 5.7. TABLE OF PHYSICAL CHARACTERISTICS OF RADIONUCLIDES MENTIONED IN THE EUROPEAN PHARMACOPOEIA Thefollowingtableisgiventocompletethegeneral monograph Radiopharmaceutical preparations (0125).
RAPPORT CEA-R-6201 MARIE-MARTINE BÉ, CHRISTOPHE DULIEU, VANESSA CHISTÉ. "NUCLÉIDE-LARA - Bibliothèque des émissions alpha, X et gamma"
RAPPORT CEA-R-6201 MARIE-MARTINE BÉ, CHRISTOPHE DULIEU, VANESSA CHISTÉ "NUCLÉIDE-LARA - Bibliothèque des émissions alpha, X et gamma" La bibliothèque NUCLÉIDE-LARA présente, pour près de 400 radionucléides
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme L iode se désintègre par émission bêta moins vers les niveaux excités de xénon, incluant l isomère xénon m de 11,962 (20) jours de période. L état d équilibre idéal, c est à dire l activité
Bookmark and Index Summary
Table of Isotopes CD- ROM Edition (Version 1.0, March 1996) The CD-ROM edition of the Table of Isotopes is an Adobe TM ACROBAT document. On- line help for ACROBAT is provided. The CD-ROM may be navigated
In your answer, you should make clear how evidence for the size of the nucleus follows from your description
1. Describe briefly one scattering experiment to investigate the size of the nucleus of the atom. Include a description of the properties of the incident radiation which makes it suitable for this experiment.
NUCLEAR WALLET CARDS
NUCLEAR WALLET CARDS (Fifth edition) JULY 1995 JAGDISH K. TULI NATIONAL NUCLEAR DATA CENTER for The U.S. Nuclear Data Network Supported by The Division of Nuclear Physics, Office of High Energy and Nuclear
Engineering Tunable Single and Dual Optical. Emission from Ru(II)-Polypyridyl Complexes. Through Excited State Design
Engineering Tunable Single and Dual Optical Emission from Ru(II)-Polypyridyl Complexes Through Excited State Design Supplementary Information Julia Romanova 1, Yousif Sadik 1, M. R. Ranga Prabhath 1,,
ΒΙΟΓΡΑΦΙΚΟ ΣΗΜΕΙΩΜΑ. Μιχελακάκης Ηλίας Michelakakis Elias Εμμανουήλ.
ΒΙΟΓΡΑΦΙΚΟ ΣΗΜΕΙΩΜΑ ΟΝΟΜΑΤΕΠΩΝΥΜΟ ΠΑΤΡΩΝΥΜΟ ΤΙΤΛΟΣ Μιχελακάκης Ηλίας Michelakakis Elias Εμμανουήλ Διδάκτωρ Φυσικός Παν/μίου Σάσσεξ Αγγλίας DPhil Doctor of Philosophy Nuclear Physics The University of Sussex
IB PHYSICS HL REVIEW PACKET: NUCLEAR PHYSICS
NAME IB PHYSICS HL REVIEW PACKET: NUCLEAR PHYSICS 1. This question is about nuclear reactions. (a) Complete the table below, by placing a tick ( ) in the relevant columns, to show how an increase in each
ƒ Š ˆ Šˆ Š Œˆ Šˆ Š ˆŒ PAMELA ˆ AMS-02
ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ 2017.. 48.. 5.. 582Ä588 œ ˆ Œ ˆ Š Ÿ Š Œ ƒ Š ˆ Šˆ Š Œˆ Šˆ Š ˆŒ PAMELA ˆ AMS-02.. ² ± 1, Š. Œ. ²μͱ 2,.. μ μ³μ²μ 1,. ˆ. Ê 2,.Œ.ƒ ²Ó 2,.. Ê 1,.. Š ²²μ 1, 2,.. ŠÊ Íμ 1,,.. ʱÓÖ μ 1,. ƒ. Œ
Appendix B Table of Radionuclides Γ Container 1 Posting Level cm per (mci) mci
3 H 12.35 Y β Low 80 1 - - Betas: 19 (100%) 11 C 20.38 M β+, EC Low 400 1 5.97 13.7 13 N 9.97 M β+ Low 1 5.97 13.7 Positrons: 960 (99.7%) Gaas: 511 (199.5%) Positrons: 1,199 (99.8%) Gaas: 511 (199.6%)
Fundamental Physical Constants Extensive Listing Relative std. Quantity Symbol Value Unit uncert. u r
UNIVERSAL speed of light in vacuum c, c 0 299 792 458 m s 1 exact magnetic constant µ 0 4π 10 7 N A 2 = 12.566 370 614... 10 7 N A 2 exact electric constant 1/µ 0 c 2 ɛ 0 8.854 187 817... 10 12 F m 1 exact
Derivation of Optical-Bloch Equations
Appendix C Derivation of Optical-Bloch Equations In this appendix the optical-bloch equations that give the populations and coherences for an idealized three-level Λ system, Fig. 3. on page 47, will be
Nuclear Physics 5. Name: Date: 8 (1)
Name: Date: Nuclear Physics 5. A sample of radioactive carbon-4 decays into a stable isotope of nitrogen. As the carbon-4 decays, the rate at which the amount of nitrogen is produced A. decreases linearly
Nuclear Data Sheets for A = 102
Nuclear Data Sheets 110 (2009) 1745 1915 www.elsevier.com/locate/nds Nuclear Data Sheets for A = 102 D. DE FRENNE University Ghent Vakgroep Subatomaire en Stralingsfysica Proeftuinstraat 86, B 9000 Gent,
«Βασικές Αρχές της SPECT και PET Απεικόνισης»
Βασικές Αρχές Πυρηνικής Ιατρικής «Βασικές Αρχές της SPECT και PET Απεικόνισης» Ι. Τσούγκος Εργαστήριο Ιατρικής Φυσικής, Παν/μιο Θεσσαλίας ΙΣΤΟΡΙΚΗ ΑΝΑΔΡΟΜΗ 1896: Henry Becquerel και το ζεύγος Curie ήταν
ˆŒ œ ƒ ƒ ˆ ˆŸ ˆ Š ˆ 137 Cs Š ˆ Œ.
Ó³ Ÿ. 2017.. 14, º 6(211).. 630Ä636 ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ. Š ˆŒ ˆ Š ˆŸ ˆŸ ˆŒ œ ƒ ƒ ˆ ˆŸ ˆ Š ˆ 137 Cs Š ˆ Œ. œ.., 1,.. ³,. ƒ. Š ² ±μ,.. ³ ±,.. ³ μ,. ˆ. É ²μ,. ˆ. ÕÉÕ ±μ, ƒ.. Ë,, ˆ.. ±μ ˆ É ÉÊÉ μ Ð Ë ± ³.. Œ.
MSWD = 1.06, probability = 0.39
MSWD Institute of Geophysics and Planetary Physics Incremental Heating 36Ar(a) 37Ar(ca) 38Ar(cl) 39Ar(k) 40Ar(r) Age (Ma) 40Ar(r) (%) 1B15835D 670 C 4 0.000001 0.078288 0.000010 0.001470 0.010633 9.19
Nuclear Data Sheets for A = 110 *
Nuclear Data Sheets 89, 481 (2000) doi:10.1006/ndsh.2000.0004 Nuclear Data Sheets for A = 110 * D. DE FRENNE AND E. JACOBS Vakgroep Subatomaire E(n) Stralingsfysica Proeftuinstraat 86, β 9000 Gent, Belgium
Fundamental Physical Constants Extensive Listing Relative std. Quantity Symbol Value Unit uncert. u r
UNIVERSAL speed of light in vacuum c, c 0 299 792 458 m s 1 exact magnetic constant µ 0 4π 10 7 N A 2 = 12.566 370 614... 10 7 N A 2 exact electric constant 1/µ 0 c 2 ɛ 0 8.854 187 817... 10 12 F m 1 exact
ΓΕΝΙΚΟΙ ΠΙΝΑΚΕΣ - TABLEAUX GENERAUX - GENERAL REPORTS
ΘΝΙΚΗ ΣΤΑΤΙΣΤΙΚΗ ΪΙΙΗΡ1ΣΙΑ ΤΗΣ Lht-Miti Β Ι Β Λ Ι Ο Θ Η Κ Η Αύξ. Άριθ. \ Κατηγ. Βιβλίου \ ΓΕΝΙΚΟΙ ΠΙΝΑΚΕΣ - TABLEAUX GENERAUX - GENERAL REPORTS Ποσότης και αξία πάντων των εισαχθέντων και εξαχθέντων εμπορευμάτων
NUCLEAR WALLET CARDS
NUCLEAR WALLET CARDS April 2005 Jagdish K. Tuli National Nuclear Data Center www.nndc.bnl.gov Brookhaven National Laboratory P.O. Box 5000 Upton, New York 11973 5000 U.S.A. Disclaimer This report was prepared
FORMULAS FOR STATISTICS 1
FORMULAS FOR STATISTICS 1 X = 1 n Sample statistics X i or x = 1 n x i (sample mean) S 2 = 1 n 1 s 2 = 1 n 1 (X i X) 2 = 1 n 1 (x i x) 2 = 1 n 1 Xi 2 n n 1 X 2 x 2 i n n 1 x 2 or (sample variance) E(X)
A life-table metamodel to support management of data deficient species, exemplified in sturgeons and shads. Electronic Supplementary Material
A life-table metamodel to support management of data deficient species, exemplified in sturgeons and shads Electronic Supplementary Material Ivan Jarić 1,2*, Jörn Gessner 1 and Mirjana Lenhardt 3 1 Leibniz-Institute
Αντιµετώπιση µετεµφραγµατικών ασθενών Αναστάσιος Λύρας Καρδιολόγος
ΟΜΑΔΑ ΕΡΓΑΣΙΑΣ ΟΞΕΩΝ ΙΣΧΑΙΜΙΚΩΝ ΣΥΝΔΡΟΜΩΝ Αντιµετώπιση µετεµφραγµατικών ασθενών Αναστάσιος Λύρας Καρδιολόγος Δεν υπάρχει σύγκρουση συµφερόντων Αντιµετώπιση µετεµφραγµατικών ασθενών Σύνολο πληθυσµού µε
Bundle Adjustment for 3-D Reconstruction: Implementation and Evaluation
3 2 3 2 3 undle Adjustment or 3-D Reconstruction: Implementation and Evaluation Yuuki Iwamoto, Yasuyuki Sugaya 2 and Kenichi Kanatani We describe in detail the algorithm o bundle adjustment or 3-D reconstruction
ΘΕΡΜΟΚΗΠΙΑΚΕΣ ΚΑΛΛΙΕΡΓΕΙΕΣ ΕΚΤΟΣ ΕΔΑΦΟΥΣ ΘΡΕΠΤΙΚΑ ΔΙΑΛΥΜΑΤΑ
ΘΕΡΜΟΚΗΠΙΑΚΕΣ ΚΑΛΛΙΕΡΓΕΙΕΣ ΕΚΤΟΣ ΕΔΑΦΟΥΣ ΘΡΕΠΤΙΚΑ ΔΙΑΛΥΜΑΤΑ Θρεπτικό διάλυμα Είναι ένα αραιό υδατικό διάλυμα όλων των θρεπτικών στοιχείων που είναι απαραίτητα για τα φυτά, τα οποία βρίσκονται διαλυμένα
[2] T.S.G. Peiris and R.O. Thattil, An Alternative Model to Estimate Solar Radiation
![[2] T.S.G. Peiris and R.O. Thattil, An Alternative Model to Estimate Solar Radiation](/thumbs/74/71129035.jpg "[2] T.S.G. Peiris and R.O. Thattil, An Alternative Model to Estimate Solar Radiation")
References [1] B.V.R. Punyawardena and Don Kulasiri, Stochastic Simulation of Solar Radiation from Sunshine Duration in Srilanka [2] T.S.G. Peiris and R.O. Thattil, An Alternative Model to Estimate Solar
2.1
181 8588 2 21 1 e-mail: sekig@th.nao.ac.jp 1. G ab kt ab, (1) k 8pGc 4, G c 2. 1 2.1 308 2009 5 3 1 2) ( ab ) (g ab ) (K ab ) 1 2.2 3 1 (g ab, K ab ) 1 t a S n a a b a 2.3 a b i (t a ) 2 1 2.4 1 g ab ab
ΤΡΙΤΕΚΝΟΣ ΠΙΝΑΚΑΣ ΚΛΑΔΟΥ
112 134 ΑΒΑΤΑΓΓΕΛΟΥ ΣΟΦΙΑ ΣΠΥΡΙΔΩΝΑΣ ΚΑΣΣΙΑΝΗ ΠΕ70 Δάσκαλοι ΟΧΙ Β 150 19 Κέρκυρα ΔΙΕΥΘΥΝΣΗ Π.Ε. ΚΕΡΚΥΡΑΣ 32 35 ΑΒΡΑΜΙΔΟΥ ΜΑΡΙΚΑ ΔΗΜΗΤΡΙΟΣ ΣΟΦΙΑ ΠΕ70 Δάσκαλοι ΟΧΙ Β 42 28,133 Ζάκυνθος ΔΙΕΥΘΥΝΣΗ Π.Ε. ΖΑΚΥΝΘΟΥ
NUCLEAR WALLET CARDS
NUCLEAR WALLET CARDS October 2011 Jagdish K. Tuli National Nuclear Data Center www.nndc.bnl.gov Brookhaven National Laboratory P.O. Box 5000 Upton, New York 11973 5000 U.S.A. Disclaimer This report was
(1) Describe the process by which mercury atoms become excited in a fluorescent tube (3)
Q1. (a) A fluorescent tube is filled with mercury vapour at low pressure. In order to emit electromagnetic radiation the mercury atoms must first be excited. (i) What is meant by an excited atom? (1) (ii)
ΟΡΙΣΤΙΚΟΣ ΠΙΝΑΚΑΣ ΩΦΕΛΟΥΜΕΝΩΝ (ΑΛΦΑΒΗΤΙΚΑ) ΑΝΑ ΔΗΜΟ ΔΟΜΗΣ
ΑΓΓΕΛΟΥ ΑΘΑΝΑΣΙΑ - ΜΑΡΙΑ 22900 74,33 ΑΓΓΕΛΟΥ ΦΙΛΙΠΠΑ - ΑΡΓΥΡΩ 20191 Α1.1 - Βρεφονηπιακός Σταθμός "Η παρεούλα μας" ΑΓΓΕΛΟΥ ΑΝΑΣΤΑΣΙΑ 83231 87,77 ΒΙΡΛΑΣ ΙΩΑΝΝΗΣ 21836 Γ - Κοινωνική Προσπάθεια (ΚΔΑΠ) (Α'
NIVEAUX C1&C2 sur l échelle proposée par le Conseil de l Europe
ΥΠΟΥΡΓΕΙΟ ΠΑΙΔΕΙΑΣ ΚΑΙ ΘΡΗΣΚΕΥΜΑΤΩΝ ΚΡΑΤΙΚΟ ΠΙΣΤΟΠΟΙΗΤΙΚΟ ΓΛΩΣΣΟΜΑΘΕΙΑΣ MINISTÈRE DE L ÉDUCATION ET DES CULTES CERTIFICATION EN LANGUE FRANÇAISE NIVEAUX C1&C2 sur l échelle proposée par le Conseil de l
Fundamental Physical Constants Complete Listing Relative std. Quantity Symbol Value Unit uncert. u r
UNIVERSAL speed of light in vacuum c, c 0 299 792 458 m s 1 (exact) magnetic constant µ 0 4π 10 7 NA 2 = 12.566 370614... 10 7 NA 2 (exact) electric constant 1/µ 0 c 2 ε 0 8.854 187 817... 10 12 Fm 1 (exact)
Butadiene as a Ligand in Open Sandwich Compounds
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2018 Butadiene as a Ligand in Open Sandwich Compounds Qunchao Fan, a Jia Fu, a Huidong
Φύλλο1. ΠΕΡΙΟΧΗ ΠΡΟΣΛΗΨΗΣ ΑΒΡΑΜΙΔΟΥ ΜΑΡΙΚΑ ΔΗΜΗΤΡΙΟΣ Γ Αθηνών ΑΒΡΑΜΙΔΟΥ ΣΟΦΙΑ ΔΗΜΗΤΡΙΟΣ Λασίθι ΑΓΓΕΛΗ ΑΝΔΡΟΜΑΧΗ ΒΑΣΙΛΕΙΟΣ
ΕΠΩΝΥΜΟ ΟΝΟΜΑ ΠΑΤΡΩΝΥΜΟ ΠΕΡΙΟΧΗ ΠΡΟΣΛΗΨΗΣ ΑΒΡΑΜΙΔΟΥ ΜΑΡΙΚΑ ΔΗΜΗΤΡΙΟΣ Γ Αθηνών ΑΒΡΑΜΙΔΟΥ ΣΟΦΙΑ ΔΗΜΗΤΡΙΟΣ Λασίθι ΑΓΓΕΛΗ ΑΝΔΡΟΜΑΧΗ ΒΑΣΙΛΕΙΟΣ Α Ανατ. Αττικής ΑΓΓΕΛΟΠΟΥΛΟΥ ΚΩΝΣΤΑΝΤΙΝΑ ΠΑΝΑΓΙΩΤΗΣ Αχαία ΑΓΓΕΛΟΠΟΥΛΟΥ
Studies on the Binding Mechanism of Several Antibiotics and Human Serum Albumin
2005 63 Vol. 63, 2005 23, 2169 2173 ACTA CHIMICA SINICA No. 23, 2169 2173 a,b a a a *,a ( a 130012) ( b 133002), 26 K A 1.98 10 4, 1.01 10 3, 1.38 10 3, 5.97 10 4 7.15 10 4 L mol 1, n 1.16, 0.86, 1.19,
ΠΑΥΛΙΝΑ 609315 ΠΕ11 25,5 ΚΑΒΑΛΑΣ ΑΝΑΤ. ΑΤΤΙΚΗ
ΕΛΛΕΙΜΑΤΙΚΕΣ - ΠΛΕΟΝΑΣΜΑΤΙΚΕΣ 1 1 ΑΒΑΝΙΔΗ ΑΝΝΑ 593587 ΠΕ70 14 ΚΟΡΙΝΘΙΑ Α ΑΘΗΝΩΝ 2 ΑΒΕΡΚΙΑΔΟΥ ΠΑΤΑΡΙΝΣΚΑ ΠΑΥΛΙΝΑ 609315 ΠΕ11 25,5 ΚΑΒΑΛΑΣ ΑΝΑΤ. ΑΤΤΙΚΗ 3 ΑΒΟΥΡΗ ΑΙΚΑΤΕΡΙΝΗ 590405 ΠΕ16 36,917 ΖΑΚΥΝΘΟΣ ΣΕΡΡΕΣ
! "#" "" $ "%& ' %$(%& % &'(!!")!*!&+ ,! %$( - .$'!"
! "#" "" $ "%& ' %$(%&!"#$ % &'(!!")!*!&+,! %$( -.$'!" /01&$23& &4+ $$ /$ & & / ( #(&4&4!"#$ %40 &'(!"!!&+ 5,! %$( - &$ $$$".$'!" 4(02&$ 4 067 4 $$*&(089 - (0:;
ˆ ˆˆ Œˆ C Z =47 50 Œ Œ ˆ ˆ Œ ˆ 23 ŒÔ
P15-2014-58.. Š ³Ö,.. ŠÔ μ²² 1,.. ± μ,.. ²Ó,. ƒ. ²μ, ƒ.. μ ±μ,.. ³ É, ƒ. Ÿ. É μ Ê ˆ ˆ ˆ ˆ Œ ˆ ˆˆ Œˆ C Z =47 50 Œ Œ ˆ ˆ Œ ˆ 23 ŒÔ ² μ Ê ² Ÿ Ö Ë ± E-mail: karamian@nrmail.jinr.ru 1 ˆ ² μ É ²Ó ± Ö ² μ Éμ
S
MSWD Institute of Geophysics and Planetary Physics Incremental Heating 36Ar(a) 37Ar(ca) 38Ar(cl) 39Ar(k) 40Ar(r) Age (Ma) 40Ar(r) (%) 1B16079D 600 C 4 0.000034 0.033821 0.000003 0.001780 0.001016 0.72
Εξωτερικός Έλεγχος Ποιότητας (External Quality Audit) στην Ακτινοθεραπεία στην Ελλάδα. Κώστας Ι. Χουρδάκης Ελληνική Επιτροπή Ατομικής Ενέργειας
Εξωτερικός Έλεγχος Ποιότητας (External Quality Audit) στην Ακτινοθεραπεία στην Ελλάδα Κώστας Ι. Χουρδάκης Ελληνική Επιτροπή Ατομικής Ενέργειας Θεσσαλονίκη, 13 Απριλίου 2014 Εργαλεία Ποιότητας Διασφάλιση
Quantitative chemical analyses of rocks with X-ray fluorescence analyzer: major and trace elements in ultrabasic rocks
98 Scientific Note X : Quantitative chemical analyses of rocks with X-ray fluorescence analyzer: major and trace elements in ultrabasic rocks Kimiko Seno and Yoichi Motoyoshi,**- +, +, ;,**. -,/ Abstract:
Hours Monday Tuesday Wednesday Thursday Friday. Physics of Diagnostic Radiology. Physics of Diagnostic Radiology. Physics of Diagnostic Radiology
Second Term, Week 1 11 15 January 2010 EXAMS Physiology EXAMS Physiology EXAMS Physiology (16h): G. Panayiotakis, G. Kandarakis Lectures will be given at Computer Lab, 1 st floor, building of the School
Supporting Information To. Microhydration of caesium compounds: Journal of Molecular Modeling
Supporting Information To Microhydration of caesium compounds: Cs, CsOH, CsI and Cs 2 I 2 complexes with one to three H 2 O molecules of nuclear safety interest Journal of Molecular Modeling Mária Sudolská
Supplementary Materials for. Kinetic and Computational Studies on Pd(I) Dimer- Mediated Halogen Exchange of Aryl Iodides
Supplementary Materials for Kinetic and Computational Studies on Pd(I) Dimer- Mediated Halogen Exchange of Aryl Iodides Indrek Kalvet, a Karl J. Bonney, a and Franziska Schoenebeck a * a Institute of Organic
Supporting Information. Crown Ether Complexes of Actinyls: A Computational Assessment of
Electronic Supplementary Material (ESI) for Dalton Transactions. This journal is The Royal Society of Chemistry 2017 Supporting Information Crown Ether Complexes of Actinyls: A Computational Assessment
ˆ ˆŸ ˆ ˆŸ ˆ ˆŒ ˆˆ Ÿ Œˆ 10 B
Ó³ Ÿ. 2013.. 10, º 4(181).. 566Ä571 ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ. Š ˆŒ ˆ ˆŸ ˆ ˆŸ ˆ ˆŒ ˆˆ Ÿ Œˆ 10 B.. ˆ μ, ˆ.. μ ±μ,.. ŠÊ Ó³ μ,.. ³ μ,. ˆ. Î,.. ÖÎ±μ ²Ó μ μ Ê É μ Ê É μ ÖÉ ƒμ Ê É Ò ÊÎ Ò Í É μ ±μ Í Ä ±μ-ô É Î ± É ÉÊÉ
Ingenieurbüro Frank Blasek - Beratender Ingenieur Am Kohlhof 10, Osterholz-Scharmbeck Tel: 04791/ Fax: 04791/
Page: 10 CONTENTS Contents... 10 General Data... 10 Structural Data des... 10 erials... 10 Sections... 10 ents... 11 Supports... 11 Loads General Data... 12 LC 1 - Vollast 120 km/h 0,694 kn/qm... 12 LC,
Ingenieurbüro Frank Blasek - Beratender Ingenieur Am Kohlhof 10, Osterholz-Scharmbeck Tel: 04791/ Fax: 04791/
Page: 1 CONTENTS Contents... 1 General Data... 1 Structural Data des... 1 erials... 1 Sections... 1 ents... 2 Supports... 2 Loads General Data... 3 LC 1 - Vollast 90 km/h 0,39 kn/qm... 3 LC, LG Results
ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ Ä664
ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ 2017.. 48.. 5.. 653Ä664 ˆ Œ ˆ ˆ e + e K + K nπ (n =1, 2, 3) Š Œ ŠŒ -3 Š - ˆ Œ Š -2000 ƒ.. μéμ Î 1,2, μé ³ ±μ²² μ Í ŠŒ -3: A.. ß ±μ 1,2,. Œ. ʲÓÎ ±μ 1,2,.. ̳ ÉÏ 1,2,.. μ 1,.. ÏÉμ μ 1,.
Supporting Information for Substituent Effects on the Properties of Borafluorenes
Supporting Information for Substituent Effects on the Properties of Borafluorenes Mallory F. Smith, S. Joel Cassidy, Ian A. Adams, Monica Vasiliu, Deidra L. Gerlach, David Dixon*, Paul A. Rupar* Department
ΑΛΚΑΛΟΕΙΔΩΝ ΘΡΥΠΤΟΦΑΝΗΣ ΑΛΕΞΑΝΔΡΟΣ Λ. ΖΩΓΡΑΦΟΣ
ΧΗΜΕΙΑ ΦΥΣΙΚΩΝ ΠΡΟΪΟΝΤΩΝ-ΒΙΟΣΥΝΘΕΣΗ ΑΛΚΑΛΟΕΙΔΩΝ ΘΡΥΠΤΟΦΑΝΗΣ ΒΙΟΣΥΝΘΕΣΗ ΑΛΚΑΛΟΕΙΔΩΝ ΘΡΥΠΤΟΦΑΝΗΣ Η L-θρυπτοφάνη είναι ένα αρωματικό αμινοξύ το οποίο φέρει ένα ινδολικό δακτύλιο και προέρχεται από το βιοσυνθετικό
ICC-ASP/7/Res.6 ICC-ASP/10/20. ISBN No All rights reserved Printed by Ipskamp, The Hague
. ICC-ASP/7/Res.6 Secretariat, Assembly of States Parties International Criminal Court P.O. Box 19519 2500 CM The Hague The Netherlands asp@asp.icc-cpi.int www.icc-cpi.int ISBN No. 92-9227-247-0 All rights
X g 1990 g PSRB
e-mail: shibata@provence.c.u-tokyo.ac.jp 2005 1. 40 % 1 4 1) 1 PSRB1913 16 30 2) 3) X g 1990 g 4) g g 2 g 2. 1990 2000 3) 10 1 Page 1 5) % 1 g g 3. 1 3 1 6) 3 S S S n m (1/a, b k /a) a b k 1 1 3 S n m,
Gro wth Properties of Typical Water Bloom Algae in Reclaimed Water
31 1 2010 1 ENVIRONMENTAL SCIENCE Vol. 31,No. 1 Jan.,2010, 3, (,, 100084) :,.,, ( Microcystis aeruginosa),3 (A 2 O ) 10 6 ml - 1,> 0139 d - 1. A 2 O222,. TP ( K max ) ( R max ), Monod. :; ; ; ; :X173 :A
Heavier chalcogenone complexes of bismuth(iii)trihalides: Potential catalysts for acylative cleavage of cyclic ethers. Supporting Information
Electronic Supplementary Material (ESI) for RSC Advances. This journal is The Royal Society of Chemistry 2015 Heavier chalcogenone complexes of bismuth(iii)trihalides: Potential catalysts for acylative
Fused Bis-Benzothiadiazoles as Electron Acceptors
Fused Bis-Benzothiadiazoles as Electron Acceptors Debin Xia, a,b Xiao-Ye Wang, b Xin Guo, c Martin Baumgarten,*,b Mengmeng Li, b and Klaus Müllen*,b a MIIT Key Laboratory of ritical Materials Technology
Laser. Light Amplification by Stimulation Emission of Radiation Ενισχυση του φωτός από ενεργοποιημένη εκπομπή ακτινοβολίας
Laser Light Amplification by Stimulation Emission of Radiation Ενισχυση του φωτός από ενεργοποιημένη εκπομπή ακτινοβολίας 50 χρόνια laser Εφαρμογές των Laser στην καθημερινότητα, στην τεχνολογία στην
Nuclear Data Sheets for A = 84 *
Nuclear Data Sheets 81, 331 (1997) Article No. DS970013 Nuclear Data Sheets for A = 8 * J. K. TULI National Nuclear Data Center Brookhaven National Laboratory Upton, NY 11973 5000, USA (Received May 22,
Laboratory Studies on the Irradiation of Solid Ethane Analog Ices and Implications to Titan s Chemistry
Laboratory Studies on the Irradiation of Solid Ethane Analog Ices and Implications to Titan s Chemistry 5th Titan Workshop at Kauai, Hawaii April 11-14, 2011 Seol Kim Outer Solar System Model Ices with
P ² Ì μ Š ˆ Œˆ Š Œ Œˆ. ² μ Ê ² Nuclear Instruments and Methods in Physics Research.
P1-2017-59.. ² Ì μ ˆ Š ˆ ˆ ƒˆ ˆˆ γ-š ƒ Œˆ Š ˆ Œˆ Š Œ Œˆ ² μ Ê ² Nuclear Instruments and Methods in Physics Research. Section A E-mail: zalikhanov@jinr.ru ² Ì μ.. P1-2017-59 μ ÒÏ ÔËË ±É μ É É Í γ-± Éμ μ
Parts Manual. Trio Mobile Surgery Platform. Model 1033
Trio Mobile Surgery Platform Model 1033 Parts Manual For parts or technical assistance: Pour pièces de service ou assistance technique : Für Teile oder technische Unterstützung Anruf: Voor delen of technische
Ó³ Ÿ , º 4Ä5(174Ä175).. 629Ä634 ˆ ˆŠ ˆ ˆŠ Š ˆ. .. Ëμ μ,.. μ, Š.. ±μ. Î ± É ÉÊÉ ³..., Œμ ±
Ó³ Ÿ. 2012.. 9, º 4Ä5(174Ä175).. 629Ä634 ˆ ˆŠ ˆ ˆŠ Š ˆ Ÿ Œ Ÿ.. Ëμ μ,.. μ, Š.. ±μ Î ± É ÉÊÉ ³..., Œμ ± Ö Ì μ ÊÌ É³μ Ë μ μ ² Ö ³ ± ³ ²Ó μ³ Ö μ³ Êɱ μé 0,8 μ 1,2 Œ É μ μ ³ Ê²Ó μ É μ ±μ ²ÊÎ Ô ± Éμ μ² 5 ±Ô
ΠΟΛΥ ΜΕΓΑΛΗ : ΜΕΓΑΛΗ : ΜΕΣΑΙΑ: ΜΙΚΡΗ
Page 1 of 67 Page 2 of 67 Page 3 of 67 Page 4 of 67 1. Page 5 of 67 Page 6 of 67 Page 7 of 67 2. Page 8 of 67 Page 9 of 67 Page 10 of 67 Page 11 of 67 Page 12 of 67 Page 13 of 67 Page 14 of 67 Page 15
Ó³ Ÿ , º 7(163).. 793Ä797 ˆ ˆŠ ˆ ˆŠ Š ˆ. .. Ëμ μ. Î ± É ÉÊÉ ³..., Œμ ±
Ó³ Ÿ. 2010.. 7, º 7(163).. 793Ä797 ˆ ˆŠ ˆ ˆŠ Š ˆ Š ˆ œ Š Œ ˆ Œ.. Ëμ μ Î ± É ÉÊÉ ³..., Œμ ± ² É Î ± ³μÉ μ Ëμ ³ μ ²Ó μéμî ÒÌ Ô² ±É μ ÒÌ Êαμ, Ö ±μéμ ÒÌ Î É Î μ É ² μ μ ³, Éμ± ³, ÒÏ ÕÐ ³ ²Ó μ Î Éμ± ²Ó. Ê
ΣΤΟΙΧΕΙΑ ΠΟΙΚΙΛΟΤΗΤΑΣ ΚΑΙ ΚΑΤΑ ΜΗΚΟΣ ΣΥΝΘΕΣΕΙΣ 4 ΕΙΔΩΝ ΨΑΡΙΩΝ ΑΝΑ ΑΛΙΕΥΤΙΚΟ ΕΡΓΑΛΕΙΟ ΣΤΟΝ ΚΕΡΚΥΡΑΪΚΟ
9 ο Πανελλήνιο Συμπόσιο Ωκεανογραφίας & Αλιείας 2009 - Πρακτικά, Τόμος ΙΙ ΣΤΟΙΧΕΙΑ ΠΟΙΚΙΛΟΤΗΤΑΣ ΚΑΙ ΚΑΤΑ ΜΗΚΟΣ ΣΥΝΘΕΣΕΙΣ 4 ΕΙΔΩΝ ΨΑΡΙΩΝ ΑΝΑ ΑΛΙΕΥΤΙΚΟ ΕΡΓΑΛΕΙΟ ΣΤΟΝ ΚΕΡΚΥΡΑΪΚΟ Παπαδοπούλου Κ.-Ν., Λιουδάκης
GS3. A liner offset equation of the volumetric water content that capacitance type GS3 soil moisture sensor measured
J. Jpn. Soc. Soil Phys. No. 130, p.19 25 (2015) GS3 1 2 A liner offset equation of the volumetric water content that capacitance type GS3 soil moisture sensor measured Shoichi MITSUISHI 1 and Masaru MIZOGUCHI
ΚΑΤΕΥΘΥΝΤΗΡΙΕΣ ΓΡΑΜΜΕΣ ΓΙΑ ΤΟΝ ΣΧΕΔΙΑΣΜΟ ΠΡΟΓΡΑΜΜΑΤΩΝ ΠΑΡΑΚΟΛΟΥΘΗΣΗΣ ΥΓΡΟΤΟΠΩΝ
ΥΠΟΥΡΓΕΙΟ ΠΕΡΙΒΑΛΛΟΝΤΟΣ ΧΩΡΟΤΑΞΙΑΣ ΚΑΙ ΔΗΜΟΣΙΩΝ ΕΡΓΩΝ ΓΕΝΙΚΗ Δ/ΝΣΗ ΠΕΡΙΒΑΛΛΟΝΤΟΣ Δ/ΝΣΗ ΠΕΡΙΒΑΛΛΟΝΤΙΚΟΥ ΣΧΕΔΙΑΣΜΟΥ ΚΑΤΕΥΘΥΝΤΗΡΙΕΣ ΓΡΑΜΜΕΣ ΓΙΑ ΤΟΝ ΣΧΕΔΙΑΣΜΟ ΠΡΟΓΡΑΜΜΑΤΩΝ ΠΑΡΑΚΟΛΟΥΘΗΣΗΣ ΥΓΡΟΤΟΠΩΝ Μαρία Αναγνωστοπούλου