Research article Special Issues

Ohmic contacts of Au and Ag metals to n-type GdN thin films

  • Received: 28 February 2015 Accepted: 29 April 2015 Published: 07 May 2015
  • The rare-earth nitrides appear as attractive alternatives to dilute ferromagnetic semiconductors for spintronics device applications. Most of them combine the properties of the ferromagnet and the semiconductor, an exceedingly rare combination. In this work we have grown n-type polycrystalline semiconducting GdN layers between pre-deposited contacts made of Cr/Au and Cr/Ag. The resistivity of the GdN layers ranges from 4.4×10-4 Ωcm to 3.1×10-2 Ωcm depending on the nitrogen pressure during the growth. The electrical properties of metal/n-type GdN/metal planar junctions are investigated as a function of the temperature. The current voltage characteristics of the junctions were linear for temperatures ranging from 300 K down to 5 K, suggesting an ohmic contact between the Au or Ag metal and the n-type GdN layer.

    Citation: Felicia Ullstad, Jay R. Chan, Harry Warring, Natalie Plank, Ben Ruck, Joe Trodahl, Franck Natali. Ohmic contacts of Au and Ag metals to n-type GdN thin films[J]. AIMS Materials Science, 2015, 2(2): 79-85. doi: 10.3934/matersci.2015.2.79

    Related Papers:

  • The rare-earth nitrides appear as attractive alternatives to dilute ferromagnetic semiconductors for spintronics device applications. Most of them combine the properties of the ferromagnet and the semiconductor, an exceedingly rare combination. In this work we have grown n-type polycrystalline semiconducting GdN layers between pre-deposited contacts made of Cr/Au and Cr/Ag. The resistivity of the GdN layers ranges from 4.4×10-4 Ωcm to 3.1×10-2 Ωcm depending on the nitrogen pressure during the growth. The electrical properties of metal/n-type GdN/metal planar junctions are investigated as a function of the temperature. The current voltage characteristics of the junctions were linear for temperatures ranging from 300 K down to 5 K, suggesting an ohmic contact between the Au or Ag metal and the n-type GdN layer.


    加载中
    [1] Dhar S, Brandt O, Ramsteiner M, et al. (2005) Colossal Magnetic Moment of Gd in GaN. Phys Rev Lett 94: 037205. doi: 10.1103/PhysRevLett.94.037205
    [2] Murmu PP, Kennedy J, Williams GVM, et al. (2012) Observation of magnetism, low resistivity, and magnetoresistance in thenear-surface region of Gd implanted ZnO. Appl Phys Lett 101:082408. doi: 10.1063/1.4747525
    [3] Chen ZT, Wang L, Yang XL, et al. (2010) Mechanism of ultrahigh Mn concentration in epitaxially grown wurtzite Ga1-xMnxN. Appl Phys Lett 97: 222108. doi: 10.1063/1.3521278
    [4] Navarro-Quezada A, Stefanowicz W, Li T, et al. (2010) Embedded magnetic phases in (Ga,Fe)N: Key role of growth temperature. Phys Rev B 81: 205206. doi: 10.1103/PhysRevB.81.205206
    [5] Dobrowolska M, Tivakornsasithorn K, Liu X, et al. (2012) Controlling the Curie temperature in (Ga,Mn)As through location of the Fermi level within the impurity band. Nature Mater 11:444-449. doi: 10.1038/nmat3250
    [6] Natali F, Ruck BJ, Plank NOV, et al. (2013) Rare-earth mononitrides. Prog Mater Sci 58:1316-1360. doi: 10.1016/j.pmatsci.2013.06.002
    [7] Mitra C, Lambrecht WRL (2008) Magnetic exchange interactions in the gadolinium pnictides from first principles. Phys Rev B 78: 134421. doi: 10.1103/PhysRevB.78.134421
    [8] Natali F, Ruck BJ, Trodahl HJ, et al. (2013) Role of magnetic polarons in ferromagnetic GdN. Phys Rev B 87: 035202. doi: 10.1103/PhysRevB.87.035202
    [9] Senapati K, Blamire MG, Barber ZH (2011) Spin-filter Josephson junctions. Nature Mater 10:849-852. doi: 10.1038/nmat3116
    [10] Blamire MG, Pal A, Barber ZH, et al. (2013) Spin filter superconducting tunnel junctions. Proc SPIE, Spintronics V 8461.
    [11] Warring H, Ruck BJ, Trodahl HJ, et al. (2013) Electric field and photo-excited control of the carrier concentration in GdN. Appl Phys Lett 102: 132409. doi: 10.1063/1.4800455
    [12] Krishnamoorthy S, Kent T, Yang J, et al. (2013) GdN Nanoisland-Based GaN Tunnel Junctions. Nano Lett 13: 2570-2575. doi: 10.1021/nl4006723
    [13] Kandala A, Richardella A, Rench DW, et al. (2013) Growth and characterization of hybrid insulating ferromagnet-topological insulator heterostructure devices. Appl Phys Lett 103: 202409. doi: 10.1063/1.4831987
    [14] Warring H, Trodahl HJ, Plank NOV, et al. (2015) Magnetic tunnel junctions based on the intrinsic ferromagnetic semiconductor GdN. Appl. Phys. Lett. [submitted].
    [15] Scarpulla MA, Gallinat CS, Mack S, et al. (2009) GdN (111) heteroepitaxy on GaN (0001) by N2 plasma and NH3 molecular beam epitaxy. J Cryst Growth 311: 1239-1244.
    [16] Natali F, Plank NOV, Galipaud J, et al. (2010) Epitaxial growth of GdN on silicon substrate using an AlN buffer layer. J Cryst Growth 24: 3583.
    [17] Natali F, Ludbrook B, Galipaud J, et al. (2012) Epitaxial growth and properties of GdN, EuN and SmN thin films. Phys Status Solidi C 9: 605. doi: 10.1002/pssc.201100363
    [18] Granville S, Ruck BJ, Budde F, et al. (2006) Semiconducting ground state of GdN thin films. Phys Rev B 73: 35335. doi: 10.1103/PhysRevB.73.035335
    [19] Lee C-M, Warring H, Vézian S, et al. (2015) Highly resistive epitaxial Mg-doped GdN thin films. Appl Phys Lett 106: 022401
  • Reader Comments
  • © 2015 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(5136) PDF downloads(872) Cited by(1)

Article outline

Figures and Tables

Figures(5)

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog