A photoluminescence study of Cd, In and Sn in ZnO using radioisotopes Joseph Cullen, Martin Henry, Enda McGlynn Dublin City University Karl Johnston Universitat.

Slides:



Advertisements
Similar presentations
1 Mechanism for suppression of free exciton no-phonon emission in ZnO tetrapod nanostructures S. L. Chen 1), S.-K. Lee 1), D. Hongxing 2), Z. Chen 2),
Advertisements

Semiconductor Device Physics
Solid State Structure Edward A. Mottel Department of Chemistry Rose-Hulman Institute of Technology.
P461 - Semiconductors1 Semiconductors Filled valence band but small gap (~1 eV) to an empty (at T=0) conduction band look at density of states D and distribution.
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Normalized plot of n 0 /N D as a function of temperature. This plot is for N D = cm  3. Figure
CHAPTER 3 CARRIER CONCENTRATIONS IN SEMICONDUCTORS
Semiconductor Physics (Physique des semi-conducteurs)
Lecture #3 OUTLINE Band gap energy Density of states Doping Read: Chapter 2 (Section 2.3)
Lecture Jan 31,2011 Winter 2011 ECE 162B Fundamentals of Solid State Physics Band Theory and Semiconductor Properties Prof. Steven DenBaars ECE and Materials.
Lecture 2 OUTLINE Semiconductor Fundamentals (cont’d) – Energy band model – Band gap energy – Density of states – Doping Reading: Pierret , 3.1.5;
Lecture 3. Intrinsic Semiconductor When a bond breaks, an electron and a hole are produced: n 0 = p 0 (electron & hole concentration) Also:n 0 p 0 = n.
SEMICONDUCTORS.
Lecture 2 OUTLINE Important quantities Semiconductor Fundamentals (cont’d) – Energy band model – Band gap energy – Density of states – Doping Reading:
SEMICONDUCTORS Semiconductors Semiconductor devices
Semiconductor Devices 22
Optical Characterization of GaN-based Nanowires : From Nanometric Scale to Light Emitting Devices A-L. Bavencove*, E. Pougeoise, J. Garcia, P. Gilet, F.
Computational Materials Design for highly efficient In-free CuInSe 2 solar sells Yoshida Lab. Yoshimasa Tani.
Electron & Hole Statistics in Semiconductors More Details
Semiconductors. Direct bandgap semiconductors (GaAs, InGaAs, InGaAsP) The minimum of CB is directly above the maximum of VB Electro-hole pair can recombine.
ECE 250 – Electronic Devices 1 ECE 250 Electronic Device Modeling.
Basic Electronics By Asst Professor : Dhruba Shankar Ray For B.Sc. Electronics Ist Year 1.
The contribution from The contribution from photoluminescence (PL) Gordon Davies, King’s College London.
NEEP 541 Ionization in Semiconductors - II Fall 2002 Jake Blanchard.
Results Study of Carrier Dynamics in ZnSe Based Scintillators by Frequency Domain Lifetime Measurements J.Mickevičius, P.Vitta, G.Tamulaitis, A. Žukauskas.
Implantation of N-O in Diamond
Impurities & Defects, Continued More on Shallow Donors & Acceptors Amusing Answers to Exam Questions Given by Public School Students!
Solid-State Electronics Chap. 6 Instructor: Pei-Wen Li Dept. of E. E. NCU 1 Chap 6. Nonequilibrium Excess Carriers in Semiconductor  Carrier Generation.
L01 01/15/021 EE Semiconductor Electronics Design Project Spring Lecture 01 Professor Ronald L. Carter
ECE 340 Lecture 6 Intrinsic Material, Doping, Carrier Concentrations
EEE 3394 Electronic Materials Chris Ferekides Fall 2014 Week 8.
High Resolution optical spectroscopy in isotopically-pure Si using radioactive isotopes: towards a re-evaluation of deep centres Mike Thewalt 1, Karl Johnston.
Low Temperature Characteristics of ZnO Photoluminescence Spectra Matthew Xia Columbia University Advisor: Dr. Karl Johnston.
LECTURE OUTLINE Electronic Properties 2 Electronic Properties 2.
Extrinsic Semiconductors ECE Definitions Intrinsic ▫Pure ▫There are an equal number of electrons and holes Extrinsic ▫Contains impurities (donors,
Slide # 1 Variation of PL with temperature and doping With increase in temperature: –Lattice spacing increases so bandgap reduces, peak shift to higher.
Luminescence basics Types of luminescence
Band Theory of Solids In isolated atoms the electrons are arranged in energy levels.
Burnaby - Dublin - Freiberg – Manchester – Saarbrücken - ISOLDE Collaboration Spokesperson: M. Deicher Contact person: K. Johnston.
Introduction to Semiconductors
1 EE 2 Fall 2007 Class 9 slides. 2 Outline 1.Review of last class 2.Extrinsic semiconductors 3.Donor and acceptor impurities 4.Majority and minority carries.
NEEP 541 Ionization in Semiconductors Fall 2002 Jake Blanchard.
. SEMICONDUCTORS Silicon bond model: Electrons and holes;
Semiconductors with Lattice Defects
President UniversityErwin SitompulSDP 2/1 Dr.-Ing. Erwin Sitompul President University Lecture 2 Semiconductor Device Physics
Isotopic fingerprints of gold-containing luminescence centers in 28 Si Karl Johnston 1, Mike Thewalt 2, Martin Henry 3 1 ISOLDE/CERN 2 Dept of Physics,
Semiconductor Conductivity Ch. 1, S It is well-known that in semiconductors, there are Two charge carriers! Electrons  e - & Holes  e + What is a hole?
Animation Demonstration No. 2. Interaction of Light with Semiconductors Normally a semiconductor material has only a few thermally excited free electrons.
Introduction to Semiconductors CSE251. Atomic Theory Consists of Electron, proton, neutron Electron revolve around nucleus in specific orbitals/shells.
A semiconductor material cannot be viewed as a collection of non interacting atoms, each with its own individual energy levels. Because of the proximity.
Manipulation of Carrier Numbers – Doping
3/2003 Rev 1 II.3.5 – slide 1 of 23 IAEA Post Graduate Educational Course Radiation Protection and Safe Use of Radiation Sources Session II.3.5 Part IIQuantities.
ZnO appropriate optical dispersion law
“Semiconductor Physics”
Lecture 2 OUTLINE Important quantities
Impurities & Defects, Continued More on Shallow Donors & Acceptors
Absorbtion FTIR: Fourier transform infrared spectroscopy

SEMICONDUCTORS Semiconductors Semiconductor devices
3.1.4 Direct and Indirect Semiconductors
Read: Chapter 2 (Section 2.3)
Chemical Bond in Metals and Semiconductors
Lecture 2 OUTLINE Semiconductor Fundamentals (cont’d)
Semiconductor Conductivity Ch. 1, S
Basic Semiconductor Physics
Semiconductor Conductivity
Review of semiconductor physics
ECE 340 Lecture 6 Intrinsic Material, Doping, Carrier Concentrations
Impurities & Defects, Continued More on Shallow Donors & Acceptors
Types of Semiconductor Materials By Dr
Presentation transcript:

A photoluminescence study of Cd, In and Sn in ZnO using radioisotopes Joseph Cullen, Martin Henry, Enda McGlynn Dublin City University Karl Johnston Universitat des Saarlandes and CERN/ISOLDE

The nature of ZnO ZnO - semiconductor at room temperature, energy gap ~ 3.4 eV - universally n-type as-grown - p-type conduction can be obtained, but not readily Difficult to purify for growth of large single crystal boules Questions: Origin(s) of dominant n-type conduction Understanding impurities / defects

Group III impurity on Zn site should: provide one excess electron act as donor: n-type conductivity provide binding centre for e-h pairs under optical excitation Group V impurity on O site should: create a free hole act as acceptor: p-type conductivity BUT these prefer to occupy Zn sites and/or form complex defects The neighbourhood of ZnO

Proof of common donor impurity identifications Wider study of Zn-site and O-site impurities Principal experimental technique : Photoluminescence at low temperatures - in conjunction with other techniques/partners in ISOLDE collaboration Our research programme:

PL intensity Photon energy (eV) Multiplicity of lines - Various impurities - Various transition types I-lines D 0 X – neutral donor-bound excitons D + X – ionised donor bound excitons Also - DAP, eA, A 0 X

Proof of identity of common donor impurities

72 Zn 72 Ga 72 Ge 73 Ga -- -- - hr 14.1 hr 4.86 hr 73 Ge ZnO:Ga I-line identification

ZnO: 73 As → 73 Ge decay Half-life: 80.3 days

Decay of Ga-related I 8 (and I 1 )Growth of Ge-related DD 2

New results from Ga → Ge decay Ge-related luminescence observed for the first time Large spectral binding energy compared to III impurities Low thermal binding energy Similar to I-lines under stress

Nature of Ge-related luminescence? Ge on Zn site: two extra electrons per Ge atom several electron-hole recombination paths are possible we are pursuing this using Zeeman/stress Theory: Ge and Si should act as shallow double-donors Lyons et al (2009)

ZnO:In I-line identification Muller at al – APL (2007) I-9 identified with In D 0 X No evidence for D + X line Possible Cd-related weak band Is I-9 the D o X for In ? Any evidence for D + X line ? Also: does Sn behave like Ge? 111 In → 111 Cd

We examined the reverse decay path 117 Ag 72 s 117 Cd 3 h 117 In 43 m

I-9 line I-2 line Confirm Muller et al result for I-9 New results: I-2 is D + X for In No Cd or Sn signals observed ZnO: 117 Cd/In/Sn

IsotopeFitted τ ½ Tabulated τ ½ 72 Ga12.7 ± 1.5 h14.1 h 73 Ga4.9 ± 0.2 h4.76 h 73 As78 ± 3 d80.3 d 117 In43 ± 2 m43.2 m Fits to experimental data

Summary Lines I-1 and I-8 due to Ga Lines I-2 and I-9 due to In New PL line due to Ge For Zn-site impurities in ZnO Not observed:Sn counterpart of Ge line Cd counterpart of Hg line (Agne et al 2003)

Thank you! ENSAR

Zn-site impurities

R. J. Mendelsberg et al. J. Vac. Sci. Technol. B 27(3) (2009) Pb in ZnO….