Tellurium

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Tellurium

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Orbitals and Energies #

Note – these are listed in BINDING ENERGY

 

Te 3s ≈ 1006eV

Te 3p ≈ 819 eV

Te 3d ≈ 572 eV

Te 4s 168 eV

Te 4p ≈ 110 eV

Te 4d ≈ 40 eV

Na2Te by XPS: Survey spectrum with peak markers
Na2Te by XPS: Survey spectrum with peak markers

Doublet Separations #

Te 3d = 10.4 eV

Te 3p = 50.8 eV

Te 4d = 1.45 eV

XPS of Te 3d with doublet separation

Common Overlaps for Te 3d #

Ag 3p – Rn 4d – Hg 4p – Cr 2p – Fr 4d – Ir 4p – Ru 3s – W 4s – Cu LMM (Al Ka X-rays)

Te 3d region with overlapping peak markers

Auger Energies #

Note – these are listed in KINETIC ENERGY

 

Te LMM ≈ 480 eV

XPS of Te MNN Region with an Al Ka source

Common Binding Energies – Te 3d #

Species #

B.E. / eV #

Charge Ref #

Reference #

Te

573

Ef = 0 eV

Te

TeO2

TeO3

Te(OH)6

p-tolyl-TeOOH

TeCl4

TeCl2

p-methoxy-phenyl-TeCl3

(NH4)2TeCl6

TeBr4

TeI4

573.1

576.1

577.3

567.7

575.7

576.9

575.8

576.3

576.5

576.7

575.9

Au 4f (84 eV)

C 1s (284.4 eV)

InTe

GaTe

575.9

573

Au 4f (84 eV)

In2Te3

572.5

Au 4f (84 eV)

Ga2Te3

572.4

C 1s (284.5 eV)

ZnTe

Na2Te

K2TeO3

(NH4)2TeO4

573.1

572.4

575.7

576.7

C 1s (285 eV)

CdTe

572.4

C 1s (284.5 eV)

PbTe

572.1

C 1s (285 eV)

MnTe

572.9

C 1s (284.8 eV)

Theory and Background #

Tellurium is a versatile element with several important uses. It is added to alloys, such as stainless steel and copper, to improve their machinability and workability. In the electronics industry, tellurium is used in semiconductors and photovoltaic cells, which are essential components of solar panels. Additionally, it acts as a colouring agent in glass and ceramics and is used in vulcanizing rubber. In battery technology, tellurium enhances the strength and hardness of lead, making it more resistant to the corrosive effects of acid in batteries.

Experimental Advice #

XPS of tellerium is typically performed on the 3d orbitals. Potential overlaps include Ag (3p), Hg (4p), Cr (2p) and Ir (4p) though depending on the oxidation states involved, the overlap with Cr and Ir may be restricted to the Te 3d3/2 peak. The may also be an interference with the Cu LMM auger region, which is crucial to determining copper speciation. The doublet separation of Te 3d is 10.39 eV.1,2

Tellerium metal exists as a simple, well separated, doublet with a small degree of asymmetry, well separated from the most stable oxide form (TeO2).3

Tellurium Dioxide, TeO2

TeO2 isprone to x-ray induced reduciton. Whilst in our experience at HarwellXPS that this is slow for a bulk powder or thick oxide film. Those analysing thin films should take care and look to potentially minimise acquisition times to avoid analysis induced effects.

 

 

Chalcogenides

Te finds itself commonly used in it’s solid state chalcogenide form (ex. GaTe, InTe etc.) in applications relating to energy materials and thus, has been analysed thoroughly in these forms by XPS.

Te 3d binding energies are typically found below that of elemental Te, due to electronegativity differences (Te = 2.1, typical cations such as Zn, Cd, In = 1.6-1.8).*

*Pauling scale

Te 3d peaks for metallic Te(1)

Data Analysis Guidance #

Not only does the metal exhibit peak asymmetry in the Te 3d region, but also Te chalcogenides may produce a similar effect. Take care to ensure correct lineshape application in this region.

Additionally, take care when analysing the Te MNN auger, since this overlaps with the Te 3s signal and may cause erroneous calculations if determining auger parameter.

Reference Datasets #

 

Coming soon

References #

  1. Data recorded at HarwellXPS
  2. Bahl, M., et al. (1977). “X‐ray photoemission studies of tellurium and some of its compounds.” The Journal of chemical physics 66(12): 5526-5535. Read it online here.
  3. Musket, R. (1978). “Studies of clean and oxidized tellurium surfaces.” Surface science 74(2): 423-435. Read it online here.
  4. Balitskii, O. and W. Jaegermann (2006). “XPS study of InTe and GaTe single crystals oxidation.” Materials chemistry and physics 97(1): 98-101. Read it online here.
  5. Guettari, N., et al. (2003). “InxTey semiconductor thin films obtained by co-evaporation.” Thin Solid Films 431: 497-501. Read it online here.
  6. Gillan, E. G. and A. R. Barron (1997). “Chemical vapor deposition of hexagonal gallium selenide and telluride films from cubane precursors: Understanding the envelope of molecular control.” Chemistry of Materials 9(12): 3037-3048. Read it online here.
  7. Poirier, D. and J. Weaver (1993). “CdTe (110) by XPS.” Surface Science Spectra 2(3): 209-216. Read it online here.
  8. Sartz, W. E., et al. (1971). “X-ray photoelectron spectroscopic investigation of Group VIA elements.” Analytical Chemistry 43(13): 1884-1887. Read it online here.
  9. Yashina, L., et al. (2004). “The oxidation of PbTe (100) surface in dry oxygen.” Surface and Interface Analysis: An International Journal devoted to the development and application of techniques for the analysis of surfaces, interfaces and thin films 36(8): 993-996. Read it online here.
  10. Iwanowski, R., et al. (2005). “Sputter cleaning and annealing of zinc-blende MnTe surface—XPS study.” Applied Surface Science 249(1-4): 222-230. Read it online here.