Charge Extraction. Lecture 9 10/06/2011 MIT Fundamentals of Photovoltaics 2.626/2.627 Fall 2011 Prof. Tonio Buonassisi
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1 Charge Extraction Lecture 9 10/06/2011 MIT Fundamentals of Photovoltaics 2.626/2.627 Fall 2011 Prof. Tonio Buonassisi
2 2.626/2.627 Roadmap You Are Here
3 2.626/2.627: Fundamentals Every photovoltaic device must obey: Conversion Efficiency Output Energy Input Energy For most solar cells, this breaks down into: Inputs Outputs Solar Spectrum Light Absorption Charge Excitation Charge Drift/Diff usion Charge Separation Charge Collection total absorption excitation drift/diffusion separation collection
4 Liebig s Law of the Minimum S. Glunz, Advances in Optoelectronics (2007) Image by S. W. Glunz. License: CC-BY. Source: High-Efficiency Crystalline Silicon Solar Cells. Advances in OptoElectronics (2007). total absorption excitation drift/diffusion separation collection
5 Learning Objectives: Charge Extraction 1. Describe the purpose of contacts, and their most common types. 2. Describe the impact of good and poor contacts on IV characteristics. 3. Sketch the IV characteristics of Schottky and Ohmic contacts. 4. Describe what fundamental material parameters determine the IV characteristics of a contact/semiconductor junction. 5. Sketch common band alignments (Types 1, 2, 3 junctions). 6. Sketch common solar cell device architectures.
6 Contacts extract carriers from device. prevent back-diffusion of carriers into device. are studied extensively in the semiconductor industry (several good review papers) for common semiconductors. are semiconductor-specific: While fundamentals generally apply universally, the devil is in the details, and each material system requires individual optimization. are influenced heavily by surface states (i.e., repeatable surface preparation is a must!)
7 Materials Commonly Used for Contacts Metals Optically opaque. Electrically conductive. Transparent Conducting Oxides (TCOs) Optically transparent. Electrically conductive.
8 Properties of TCOs Transparency Conductivity ( ) 1 Quartz Glass Si Ge ITO Ag Transparency 0 0 Visible Energy of light (ev) -18 Insulator Semi conductor -6-2 log (S/cm) = n e 2 Metal 6 Transmittance: > 80% (Films) Range: 400 ~ 700 nm Band gap > 3.1eV n - carrier conc. (cm -3 ) - mobility (cm 2 /Vs) e - charge per carrier
9 How TCOs Work CB E E F E 1 = Large E 3 = very small E 2 = Large VB x
10 Learning Objectives: Charge Extraction 1. Describe the purpose of contacts, and their most common types. 2. Describe the impact of good and poor contacts on IV characteristics. 3. Sketch the IV characteristics of Schottky and Ohmic contacts. 4. Describe what fundamental material parameters determine the IV characteristics of a contact/semiconductor junction. 5. Sketch common band alignments (Types 1, 2, 3 junctions). 6. Sketch common solar cell device architectures.
11 Equivalent Circuit: Simple Case Lin Scale V ja J 0 V Current Density (ma/cm2) 1.E+00 8.E-01 6.E-01 4.E-01 2.E-01 0.E+00 I-V Curve Voltage (V) J J 0 exp qv 1 J kt L Current Density (ma/cm2) 1.E+00 1.E-02 1.E-04 1.E-06 1.E-08 1.E-10 Log Scale I-V Curve Voltage (V)
12 Equivalent Circuit: Simple Case V ja J 0 R s V Current Density (ma/cm2) 5.E-02 4.E-02 3.E-02 2.E-02 1.E-02 0.E+00 I-V Curve Voltage (V) J J 0 exp q V JR s kt 1 J L Current Density (ma/cm2) 1.E+00 1.E-02 1.E-04 1.E-06 1.E-08 1.E-10 I-V Curve Voltage (V)
13 Equivalent Circuit: Simple Case V ja J 0 R s R sh V Current Density (ma/cm2) 5.E-02 4.E-02 3.E-02 2.E-02 1.E-02 0.E+00 I-V Curve Voltage (V) J J 0 exp q V JR s kt 1 V JR s R sh J L Current Density (ma/cm2) 1.E+00 1.E-02 1.E-04 1.E-06 1.E-08 1.E-10 I-V Curve Voltage (V)
14 Equivalent Circuit: Simple Case R s J 0 V ja R sh V J J 0 exp q V JR s kt 1 V JR s R sh J L Courtesy of PVCDROM. Used with permission. Firing contacts? Three possibilities: 1. Contact just right: low R s, large R sh. 2. Underfired contact: Poor contact with Si, large R s. 3. Overfired contact: Metal drives too deep into Si, low R sh.
15 Learning Objectives: Charge Extraction 1. Describe the purpose of contacts, and their most common types. 2. Describe the impact of good and poor contacts on IV characteristics. 3. Sketch the IV characteristics of Schottky and Ohmic contacts. 4. Describe what fundamental material parameters determine the IV characteristics of a contact/semiconductor junction. 5. Sketch common band alignments (Type 1, 2, 3, and 4 junctions). 6. Sketch common solar cell device architectures.
16 Classes of Contacts Ohmic: Ohmic and Schottky Contacts Linear I-V curve. Typically used when charge separation is not a goal for metallization. Schottky: Current (a.u.) + 0 Schottky Ohmic Exponential I-V curve. - Used when charge separation is desired Voltage (a.u.)
17 Learning Objectives: Charge Extraction 1. Describe the purpose of contacts, and their most common types. 2. Describe the impact of good and poor contacts on IV characteristics. 3. Sketch the IV characteristics of Schottky and Ohmic contacts. 4. Describe what fundamental material parameters determine the IV characteristics of a contact/semiconductor junction. 5. Sketch common band alignments (Types 1, 2, 3 junctions). 6. Sketch common solar cell device architectures.
18 Step #1: Schottky Theory (the ideal case)
19 Contacts: Schottky Model E Vacuum E C q c q f M E F E V x Semiconductor Metal
20 Contacts: Schottky Model E Vacuum q c q f M E C E F E V x Semiconductor Metal
21 Contacts: Schottky Model For Ohmic contact: f m > f s Barrier Height: f b = f m - c Contact Potential: V bi = f m - f s Space-charge region width: W 2 s qn D V o Courtesy of Tesfaye Ayalew. Used with permission.
22 Classes of Contacts Ohmic: Electron barrier height 0 (for n-type) Linear I-V curve. Typically used when charge separation is not a goal for metallization. Schottky: Electron barrier height > 0 (for p-type) Exponential I-V curve. Used when charge separation is desired. Current (a.u.) Ohmic and Schottky Contacts Voltage (a.u.) Schottky Ohmic
23 Evaluating Metals for Contacts - Schottky Model Courtesy of Tesfaye Ayalew. Used with permission.
24 Reality: Deviations from Schottky theory Substantial deviations from Schottky theory are possible, due to interface effects including: Orientation-dependent surface states. Elemental nature of surface termination in binary compounds (e.g., A or B element?). Interface dipoles. and more Courtesy of Tesfaye Ayalew. Used with permission.
25 Role of Surface States For related visuals, please see the lecture 9 video or the reference below. D.K. Schroder, IEEE Trans. Electron Dev. 31, 637 (1984)
26 Contacts: Schottky Model For Ohmic contact: f m > f s Barrier Height: f b = f m - c Contact Potential: V bi = f m - f s Space-charge region width: W 2 s qn D V o Courtesy of Tesfaye Ayalew. Used with permission.
27 Thermionic Emission & Field Emission Effects For related visuals, please see the lecture 9 video or the reference below. D.K. Schroder, IEEE Trans. Electron Dev. 31, 637 (1984)
28 Evaluating Metals for Contacts - Practical Sources: Reference books Review articles Scientific articles Trusted websites NB: Surface states matter!! Be sure you have repeatable surface preparation.
29 Learning Objectives: Charge Extraction 1. Describe the purpose of contacts, and their most common types. 2. Describe the impact of good and poor contacts on IV characteristics. 3. Sketch the IV characteristics of Schottky and Ohmic contacts. 4. Describe what fundamental material parameters determine the IV characteristics of a contact/semiconductor junction. 5. Sketch common band alignments (Types 1, 2, 3 junctions). 6. Sketch common solar cell device architectures.
30 Evaluating Heterojunctions Not always possible to dope a material both n- and p-type. Not always possible to find the perfect contact material. Need: heterojunction. (At least) three types of heterojunction: What junction will separate charge?
31 Evaluating Heterojunctions E Simplest case (analogy to Schottky band alignment for metalsemiconductor contacts): 1- Set chemical potential equal across entire device. 2- Then, align vacuum levels. 3- Note that VB and CB must follow vacuum levels. x
32 Evaluating Heterojunctions Simplest case (analogy to Schottky band alignment for metalsemiconductor contacts): 1- Set chemical potential equal across entire device. 2- Then, align vacuum levels. 3- Note that VB and CB must follow vacuum levels.
33 MIT OpenCourseWare / Fundamentals of Photovoltaics Fall 2013 For information about citing these materials or our Terms of Use, visit:
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