These tools will no longer be maintained as of December 31, 2024. Archived website can be found here. PubMed4Hh GitHub repository can be found here. Contact NLM Customer Service if you have questions.


BIOMARKERS

Molecular Biopsy of Human Tumors

- a resource for Precision Medicine *

292 related articles for article (PubMed ID: 17501373)

  • 1. Dual character of the electronic structure of YBa2Cu4O8: the conduction bands of CuO2 planes and CuO chains.
    Kondo T; Khasanov R; Karpinski J; Kazakov SM; Zhigadlo ND; Ohta T; Fretwell HM; Palczewski AD; Koll JD; Mesot J; Rotenberg E; Keller H; Kaminski A
    Phys Rev Lett; 2007 Apr; 98(15):157002. PubMed ID: 17501373
    [TBL] [Abstract][Full Text] [Related]  

  • 2. Anomalies in the Fermi surface and band dispersion of quasi-one-dimensional CuO chains in the high-temperature superconductor YBa2Cu4O8.
    Kondo T; Khasanov R; Karpinski J; Kazakov SM; Zhigadlo ND; Bukowski Z; Shi M; Bendounan A; Sassa Y; Chang J; Pailhés S; Mesot J; Schmalian J; Keller H; Kaminski A
    Phys Rev Lett; 2010 Dec; 105(26):267003. PubMed ID: 21231707
    [TBL] [Abstract][Full Text] [Related]  

  • 3. Atomic scale real-space mapping of holes in YBa2Cu3O(6+δ).
    Gauquelin N; Hawthorn DG; Sawatzky GA; Liang RX; Bonn DA; Hardy WN; Botton GA
    Nat Commun; 2014 Jul; 5():4275. PubMed ID: 25023575
    [TBL] [Abstract][Full Text] [Related]  

  • 4. Parity of the pairing bosons in a high-temperature Pb-Bi2Sr2CaCu2O8 bilayer superconductor by angle-resolved photoemission spectroscopy.
    Borisenko SV; Kordyuk AA; Koitzsch A; Fink J; Geck J; Zabolotnyy V; Knupfer M; Büchner B; Berger H; Falub M; Shi M; Krempasky J; Patthey L
    Phys Rev Lett; 2006 Feb; 96(6):067001. PubMed ID: 16606032
    [TBL] [Abstract][Full Text] [Related]  

  • 5. Indirect electric field doping of the CuO2 planes of the cuprate NdBa2Cu3O7 superconductor.
    Salluzzo M; Ghiringhelli G; Cezar JC; Brookes NB; De Luca GM; Fracassi F; Vaglio R
    Phys Rev Lett; 2008 Feb; 100(5):056810. PubMed ID: 18352415
    [TBL] [Abstract][Full Text] [Related]  

  • 6. Origin of the peak-dip-hump line shape in the superconducting-state (pi,0) photoemission spectra of Bi2Sr2CaCu2O8.
    Kordyuk AA; Borisenko SV; Kim TK; Nenkov KA; Knupfer M; Fink J; Golden MS; Berger H; Follath R
    Phys Rev Lett; 2002 Aug; 89(7):077003. PubMed ID: 12190550
    [TBL] [Abstract][Full Text] [Related]  

  • 7. Enhanced superconducting gaps in the trilayer high-temperature Bi2Sr2Ca2Cu3O(10+δ) cuprate superconductor.
    Ideta S; Takashima K; Hashimoto M; Yoshida T; Fujimori A; Anzai H; Fujita T; Nakashima Y; Ino A; Arita M; Namatame H; Taniguchi M; Ono K; Kubota M; Lu DH; Shen ZX; Kojima KM; Uchida S
    Phys Rev Lett; 2010 Jun; 104(22):227001. PubMed ID: 20867198
    [TBL] [Abstract][Full Text] [Related]  

  • 8. Self-doping processes between planes and chains in the metal-to-superconductor transition of YBa2Cu3O6.9.
    Magnuson M; Schmitt T; Strocov VN; Schlappa J; Kalabukhov AS; Duda LC
    Sci Rep; 2014 Nov; 4():7017. PubMed ID: 25388860
    [TBL] [Abstract][Full Text] [Related]  

  • 9. Negative quantum interference between the electronic Raman scattering processes of CuO chains and CuO2 planes of heavily overdoped (Y, Ca)Ba2Cu3O(7-delta).
    Masui T; Limonov M; Uchiyama H; Tajima S; Yamanaka A
    Phys Rev Lett; 2005 Nov; 95(20):207001. PubMed ID: 16384088
    [TBL] [Abstract][Full Text] [Related]  

  • 10. Crossing the gap from p- to n-type doping: nature of the states near the chemical potential in La(2)-(x)Sr(x)CuO(4) and Nd(2-x)Ce(x)CuO(4-delta).
    Steeneken PG; Tjeng LH; Sawatzky GA; Tanaka A; Tjernberg O; Ghiringhelli G; Brookes NB; Nugroho AA; Menovsky AA
    Phys Rev Lett; 2003 Jun; 90(24):247005. PubMed ID: 12857219
    [TBL] [Abstract][Full Text] [Related]  

  • 11. The phase diagram of electron-doped La(2-x)Ce(x)CuO(4-δ).
    Saadaoui H; Salman Z; Luetkens H; Prokscha T; Suter A; MacFarlane WA; Jiang Y; Jin K; Greene RL; Morenzoni E; Kiefl RF
    Nat Commun; 2015 Jan; 6():6041. PubMed ID: 25608106
    [TBL] [Abstract][Full Text] [Related]  

  • 12. Three- to two-dimensional transition of the electronic structure in CaFe2As2: a parent compound for an iron arsenic high-temperature superconductor.
    Liu C; Kondo T; Ni N; Palczewski AD; Bostwick A; Samolyuk GD; Khasanov R; Shi M; Rotenberg E; Bud'ko SL; Canfield PC; Kaminski A
    Phys Rev Lett; 2009 Apr; 102(16):167004. PubMed ID: 19518747
    [TBL] [Abstract][Full Text] [Related]  

  • 13. Imaging the effects of individual zinc impurity atoms on superconductivity in Bi2Sr2CaCu2O8+delta.
    Pan SH; Hudson EW; Lang KM; Eisaki H; Uchida S; Davis JC
    Nature; 2000 Feb; 403(6771):746-50. PubMed ID: 10693798
    [TBL] [Abstract][Full Text] [Related]  

  • 14. Anomalous momentum dependence of the quasiparticle scattering rate in overdoped Bi2Sr2CaCu2O8.
    Bogdanov PV; Lanzara A; Zhou XJ; Yang WL; Eisaki H; Hussain Z; Shen ZX
    Phys Rev Lett; 2002 Oct; 89(16):167002. PubMed ID: 12398747
    [TBL] [Abstract][Full Text] [Related]  

  • 15. Proximity effects and quantum dissipation in the chains of YBa2Cu3O6+x.
    Morr DK; Balatsky AV
    Phys Rev Lett; 2001 Dec; 87(24):247002. PubMed ID: 11736531
    [TBL] [Abstract][Full Text] [Related]  

  • 16. Hybridization of Bogoliubov Quasiparticles between Adjacent CuO_{2} Layers in the Triple-Layer Cuprate Bi_{2}Sr_{2}Ca_{2}Cu_{3}O_{10+δ} Studied by Angle-Resolved Photoemission Spectroscopy.
    Ideta S; Johnston S; Yoshida T; Tanaka K; Mori M; Anzai H; Ino A; Arita M; Namatame H; Taniguchi M; Ishida S; Takashima K; Kojima KM; Devereaux TP; Uchida S; Fujimori A
    Phys Rev Lett; 2021 Nov; 127(21):217004. PubMed ID: 34860085
    [TBL] [Abstract][Full Text] [Related]  

  • 17. Bilayer splitting in the electronic structure of heavily overdoped Bi(2)Sr(2)CaCu(2)O(8+delta).
    Feng DL; Armitage NP; Lu DH; Damascelli A; Hu JP; Bogdanov P; Lanzara A; Ronning F; Shen KM; Eisaki H; Kim C; Shen ZX; Shimoyama J; Kishio K
    Phys Rev Lett; 2001 Jun; 86(24):5550-3. PubMed ID: 11415298
    [TBL] [Abstract][Full Text] [Related]  

  • 18. Electronic structure of Eu(Fe0.79Ru0.21)2As2 studied by angle-resolved photoemission spectroscopy.
    Xia M; Jiao WH; Ye ZR; Ge QQ; Zhang Y; Jiang J; Peng R; Shen XP; Fan Q; Cao GH; Zhang T; Xie BP; Feng DL
    J Phys Condens Matter; 2014 Jul; 26(26):265701. PubMed ID: 24912631
    [TBL] [Abstract][Full Text] [Related]  

  • 19. Transition metal chalcogenides: ultrathin inorganic materials with tunable electronic properties.
    Heine T
    Acc Chem Res; 2015 Jan; 48(1):65-72. PubMed ID: 25489917
    [TBL] [Abstract][Full Text] [Related]  

  • 20. Dual nature of the electronic structure of (La(2--x--y)Nd(y)Sr(x))CuO(4) and La(1.85)Sr(0.15)CuO(4).
    Zhou XJ; Yoshida T; Kellar SA; Bogdanov PV; Lu ED; Lanzara A; Nakamura M; Noda T; Kakeshita T; Eisaki H; Uchida S; Fujimori A; Hussain Z; Shen ZX
    Phys Rev Lett; 2001 Jun; 86(24):5578-81. PubMed ID: 11415305
    [TBL] [Abstract][Full Text] [Related]  

    [Next]    [New Search]
    of 15.