figure 9.1. use of silicon oxide as a masking layer during diffusion of dopants

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Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants.

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Page 1: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants.

Page 2: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.2. Evolution of integrated circuit technology.

Page 3: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.3. Moore's law (data points are for INTEL’s microprocessors; the projections are based on the 2002 Technology Roadmap ITRS02)2.

Page 4: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.4. Trend of the minimum feature size (2002 Technology Roadmap ITRS02)2.

Page 5: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.5. Average selling price per bit of DRAM memory since 19805.

Page 6: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.6. Trend of the cost per element over the years indicating the main contributing factors to the cost reduction9. 

Page 7: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.7. Clock speed of microprocessors since 19805.

Page 8: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.8. Part of the periodic table showing the III, IV, and V columns. The elemental semiconductors Si and Ge belong to column IV.

Page 9: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.9. Schematic representation of the orbital model of a single silicon atom, with its 14 electrons of which the 4 valence electrons reside

in the outermost shell. The energy levels are shown to the right (not to scale).

Page 10: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.10. (a) Tetrahedral bonding of silicon in the diamond structure showing the four nearest neighbors connected through covalent bonds; (b) 2-D bond model illustrating the sharing of the valence electrons between

nearest-neighbor silicon atoms. Each line between the silicon core represents one valence electron.

Page 11: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.11. (a) Energy levels in an isolated silicon atom and (b) in a silicon crystal of N atoms, illustrating the formation of energy bands. The

valence band contains 4N states and can accommodate all 4N valence electrons.

Page 12: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.12. A valence electron jumping across the energy gap in pure silicon resulting in the generation of a free electron and hole in the

crystal: (a) energy band model, (b) bond model.

Page 13: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.13. Extrinsic n-type silicon doped with P donor atoms. (a) Energy band diagram and (b) Bond model.

Page 14: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.14. Extrinsic p-type silicon doped with B acceptor atoms. (a) Energy band diagram and (b) Bond model.

Page 15: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.15. (a) Schematic cross-sectional view of a MOS capacitor; (b) Energy band diagram (not to scale) of the MOS capacitor under flat band

conditions along the cross section AA'.

Page 16: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.16. MOS capacitor in depletion: (a) cross section and (b) the energy band diagram along the cross section AA'.

Page 17: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.17. Schematic view of a n-type MOSFET.

Page 18: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.18. Current flow in a NMOS transistor, illustrating the three operating regions (linear, triode and saturation).

Page 19: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.19. Scaling trends in industry (data points) as compared to the trends for constant field scaling (dashed lines): (a) current per unit gate

width, delay, power density, and gate capacitance; (b) active and subthreshold power densities vs. the gate length.(From Ref. 18, courtesy of International Business Machines Corporation. Unauthorized use not

permitted.)  

Page 20: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.20. Cross section of a MOSFET showing the depletion region under the gate, source and drain. The depletion region under the gate is in part a function of the depletion region controlled by the source and drain,

causing short channel effects.

Page 21: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.21. Projection of the printed and physical gate lengths of transistors in MPUs according to the ITRS20022.

Page 22: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.22. Schematic cross section of a SOI NMOS.

Page 23: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.23. Schematic illustration of the effect of Ge atoms, implanted in a Si crystal, on the strain of Silicon. (From Ref. 25 by permission of the

Institute of Electrical and Electronics Engineers. © 2003 IEEE)

Page 24: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.24. Scaling of the physical gate dielectric thickness and effective oxide thickness (EOT), based on data from the ITRS2002. (From Ref. 4 by permission of the Institute of Electrical and Electronics Engineers. ©

2003 IEEE)

Page 25: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.25. Schematic cross sections: (a) conventional bulk MOSFET and (b) dual gate FET.

Page 26: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.26. Conceptual representation of double-gate field effect transistors [Adapted from H.-S. Wong, K. Chan, and Y. Taur, IEDM

Tech. Digest, p. 427 (1997)].

Page 27: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.27. Schematic view of a FinFET, type III double-gate FET.

Page 28: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.28. Representation of emerging technologies in a 3-D space of speed, size and cost2,37. (From Ref. 37 by permission of the Institute of

Electrical and Electronics Engineers. © 2003 IEEE )

Page 29: Figure 9.1. Use of silicon oxide as a masking layer during diffusion of dopants

Figure 9.29. Schematic cross-section of a carbon nanotube field effect transistor (CNFET). (Adapted from Ph. Avouris, Acc. Chem. Res. 35,

1026 (2002) with kind permission of Ph. Avouris.)