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1 | Nonimaging optical systems and their uses | 1 |
2 | Some basic ideas in geometrical optics | 7 |
3 | Some designs of image-forming concentrators | 25 |
4 | Nonimaging optical systems | 43 |
5 | Developments and modifications of the compound parabolic concentrator | 69 |
6 | The flow-line method for designing nonimaging optical systems | 99 |
7 | Concentrators for prescribed irradiance | 159 |
8 | Simultaneous multiple surface design method | 181 |
9 | Imaging applications of nonimaging concentrators | 219 |
10 | Consequences of symmetry | 235 |
11 | Global optimization of high-performance concentrators | 265 |
12 | A paradigm for a wave description of optical measurements | 305 |
13 | Applications to solar energy concentration | 317 |
14 | Manufacturing tolerances | 395 |
App. A | Derivation and explanation of the etendue invariant, including the dynamical analogy; derivation of the skew invariant | 415 |
App. B | The edge-ray theorem | 421 |
App. C | Conservation of skew and linear momentum | 433 |
App. D | Conservation of etendue for two-parameter bundles of rays | 439 |
App. E | Perfect off-axis imaging | 449 |
App. F | The Luneberg lens | 461 |
App. G | The geometry of the basic compound parabolic concentrator | 467 |
App. H | The [theta][subscript i]/[theta][subscript o] concentrator | 471 |
App. I | The truncated compound parabolic concentrator | 473 |
App. J | The differential equation for the 2D concentrator profile with nonplane absorber | 477 |
App. K | Skew rays in hyperboloidal concentrator | 481 |
App. L | Sine relation for hyperboliod/lens concentrator | 483 |
App. M | The concentrator design for skew rays | 485 |
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