H0

Results: 145



#Item
81Nuclear and Isotopic Techniques for the Characterization of Submarine Ground Water Discharge (SGD) in Coastal Zones Pavel P. Povinec, Sang-Han Lee, Jean-François Comanducci, Beniamino Oregioni, Isabelle Lévy-Palomo, Jo

Nuclear and Isotopic Techniques for the Characterization of Submarine Ground Water Discharge (SGD) in Coastal Zones Pavel P. Povinec, Sang-Han Lee, Jean-François Comanducci, Beniamino Oregioni, Isabelle Lévy-Palomo, Jo

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Source URL: www.iaea.org

Language: English - Date: 2009-07-24 11:28:09
82Citation: K.A. Olive et al. (Particle Data Group), Chin. Phys. C38, [removed]URL: http://pdg.lbl.gov)  H0 J = 0 In the following H 0 refers to the signal that has been discovered in

Citation: K.A. Olive et al. (Particle Data Group), Chin. Phys. C38, [removed]URL: http://pdg.lbl.gov) H0 J = 0 In the following H 0 refers to the signal that has been discovered in

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Source URL: pdg.lbl.gov

Language: English - Date: 2014-08-21 15:57:29
83Pohled na točnu po modelářské stránce dokončeného velkého depa ve velikosti H0: venku je patinováno prakticky vše, stojiny kolejnic, střechy budov i dno betonové jámy točny. S tím kontrastuje snad poněkud

Pohled na točnu po modelářské stránce dokončeného velkého depa ve velikosti H0: venku je patinováno prakticky vše, stojiny kolejnic, střechy budov i dno betonové jámy točny. S tím kontrastuje snad poněkud

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Source URL: www.railvolution.net

Language: Czech - Date: 2011-05-31 15:30:40
    84SERVICE CANTONAL DE STATISTIQUE  H0 T E L L E R I E GE NE V0 I S E

    SERVICE CANTONAL DE STATISTIQUE H0 T E L L E R I E GE NE V0 I S E

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    Source URL: www.ge.ch

    Language: English - Date: 2014-04-23 05:22:54
      85A Program Logic for Resource Verification David Aspinall1 , Lennart Beringer1 , Martin Hofmann2 , Hans-Wolfgang Loidl2 , Alberto Momigliano1 1 2

      A Program Logic for Resource Verification David Aspinall1 , Lennart Beringer1 , Martin Hofmann2 , Hans-Wolfgang Loidl2 , Alberto Momigliano1 1 2

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      Source URL: groups.inf.ed.ac.uk

      Language: English - Date: 2004-05-24 09:01:38
      86The Physics of Rock Throwing  The horizontal motion of a rock (projectile) is given by the formula: X = Vh T Independently, the vertical motion is given by the formula Y = H0 + VvT – ½ gT2

      The Physics of Rock Throwing The horizontal motion of a rock (projectile) is given by the formula: X = Vh T Independently, the vertical motion is given by the formula Y = H0 + VvT – ½ gT2

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      Source URL: spacemath.gsfc.nasa.gov

      Language: English - Date: 2014-02-06 09:56:16
      87N:H0 NYA_PPS_5525.00�s�j5.00_PPS_AR SD PLAN 11x17 (1)

      N:H0 NYA_PPS_5525.00sj5.00_PPS_AR SD PLAN 11x17 (1)

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      Source URL: ourpublicservice.org

      - Date: 2014-11-01 12:49:07
        88C/2013 V5 (Oukaimeden)  SkyTools 3 / Skyhound.com N

        C/2013 V5 (Oukaimeden) SkyTools 3 / Skyhound.com N

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        Source URL: www.cometchasing.skyhound.com

        Language: English - Date: 2014-10-01 19:27:14
        89Week 6 (due Nov. 14) Reading: Srednicki, sections 8,9,[removed]a) Consider the free real scalar field (with mass m). Use the pathintegral representation to compute the expectation values  A = h0|eiaφ(x) |0i, B(x − y)

        Week 6 (due Nov. 14) Reading: Srednicki, sections 8,9,[removed]a) Consider the free real scalar field (with mass m). Use the pathintegral representation to compute the expectation values  A = h0|eiaφ(x) |0i, B(x − y)

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        Source URL: www.theory.caltech.edu

        Language: English - Date: 2007-11-14 20:46:50
        90Week 5 (due Nov[removed]Problem[removed]Srednicki) 2. Consider free scalar field φ of mass m. Show that the Green’s function G(2) (x) = h0|T (φ(x)φ(0))|0i satisfies (−∂ 2 + m2 )G(2) (x) = −iδ 4 (x).

        Week 5 (due Nov[removed]Problem[removed]Srednicki) 2. Consider free scalar field φ of mass m. Show that the Green’s function G(2) (x) = h0|T (φ(x)φ(0))|0i satisfies (−∂ 2 + m2 )G(2) (x) = −iδ 4 (x).

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        Source URL: www.theory.caltech.edu

        - Date: 2009-10-31 19:40:01