CHEM 524 Course Outline (Sect. 4) - 2005

FOR A PDF VERSION OF THIS SET OF NOTESWITH EMBEDDED FIGURES CLICK HERE (this may not be available for download until Sept.)

 

III. Optics — Control of light — move it from source to detector through experiment

A. Lenses + Mirror (Text: Ch 3 & 1,4) design — shape & materials — efficiency

1.Basic concepts: index of refraction — n = c/v, c = 3 x 108m/s,

nglass ~ 1.5,   nCaF2 ~ 1.35,  nZnSe ~ 2.5,   nGe ~ 4 – liquids as well: nwater ~ 1.33 ,  nalcohol ~ 1.36,  nCCl4 ~ 1.466, nBr-napthalene ~ 1.659

            non-isotropic depends on direction: quartz: no ~ 1.544 ne ~ 1.553,  zircon: no ~ 1.923 ne ~ 1.968 (uniaxial crystals, o=ordinary, xx and yy,  e=extraordinary, zz)

conservation law: r(l) + a(l) + T(l) = 1 - mirror T~ 0 & lens T ~ 1

dispersion (index, n, increase with dec l) — dn(l)/dl < 0  (also dispersion generally dec. with inc. l)

(exception, if absorption band, index is complex and has singularity, derivative shape)

Snell’s law of refraction:   n, sin q1 = n2 sin q2,

reflection: q1 = q3 vs. refraction: q2 < q1 for n1 < n2

reflection loss: r(l) = (n2-n1/n2+n1)2, normal incidence, e.g. air/glass ~ 4%,   but ZnSe ~18% per surface

Brewster angle, — zero reflection loss in one polarization (II to reflection plane) at specific angle   qB = tan-1(n2/n1)

Total internal reflection, - n1>n2, r(l) max at q1=qc,   qc = sin-1(n2/n1)

air — glass,   qc ~ 42o,  useful property for prism reflectors (no coating, higher power possible)

2. Mirrors: spherical mirror imaging — reflection,

materials — Al(uv), Ag (vis), Au(IR), coating can help r  -- VUV—MgF2, vis-SiO

spherical mirror focusing: mirror formula:  2/R = 1/ S1 +1/ S2 =1/f,

S1 — object — O,   S2 — image — I,   R — radius (R<0 concave),   f — focus

S1 = infinite, parallel beam,ΰ S2 =  f,  S1 = S2 = -R  ΰ 1:1 imaging

magnification:   m = -I/0 = - S2/ S1

result:  S1 > R — demagnify, f < S1 < R — magnify, S1 < f — no image

variations: plane, convex (virtual positive image), aspherical, elliptical, parabolic, off-axis parabola

            Prism—use total internal reflection, no coating, high power

3. Lens: refraction straight line design, must transmit but losses due reflection or absorption

spectral region, material dependent:

  • quartz — uv (180nm) to near IR ~ 3 m. — 4.5 m.
  • CaF2 — vuv (140nm) to mid IR ~ 8 m.
  • ZnSe — yellow (~500 nm) to IR ~ 16 m.
  • Ge — near IR (~2 m) to IR ~ 20 m.

Thin-lens

operative formula:   1/ S1 +1/ S2 =1/f,

lens makers formula for one surface: n1/ S1 +n2/ S2 = (n2 -n1)/R,

typically purchase based on size and focal length so in practice ignore radius, but can increase efficiency by choosing best combination

magnification: same as mirror: m = -S2/S1

special designs: cylindrical (focus one dimension), aspherical (reduce aberration)

AR coating — reduce reflection loss (n — index lens, n Ε 1 air) - r=(n-1/n+1)2

-- add l/4 layer of intermediate index n1 , or multiple layers— goal: zero reflection by interference, sensitive to angle

-- multilayer (N)— get zeros at (N — 1) l’s

4. Light gather power — trade off: more light or smaller image  (m = 1 often best): 

closer to source, collect more BUT image bigger (further, brighter image, smaller spot BUT less light)

F-number: [F/n] = f/D, if not circular shape: D = (4A/p)1/2

Called the speed — smaller is faster

Irradiance (goes as square): halve F/n, quadruple light   (e.g. camera people: F/1.4 is twice the light of F/2.0)

Varies as solid angle, W,    E=Bs(p/4)/(F/n)2

5. Aberrations (solution): chromatic (compound lens, mirror), spherical (reduce aperture, plano-convex), coma (align, red. apert.), astigmatism (reduce off-axis mirror, parabolic)

B. Special

1. Fiber optics — total internal reflection — limits acceptance angle

2. Beam Splitter — divides beam in space (can be coating or just surface, can use angle to enhance, single surface best)

3. Filters — color filters are glasses with absorbing materials mixed in, ex. Salts of transition metals, band pass or cut off, progressing out to even IR

--interference — multiple layers of dielectric act as Fabry-Perot interferometer,  narrow -band or cut off:

 

Homework—read Chap 3-1, 2, 3, 4, 5 (will carry over to Section 5, Special Optics)

Problems to do: Ch 3: 2, 7, 12, 18, 26

 

Links to optics etc:

 

Melles Griot Optics tutorial (also sell optics)

http://www.mellesgriot.com/products/optics/opticaltutorial.asp

 

Newport-Oriel Optics section (also sell optics):

http://www.newport.com/Optics/1/productmain.aspx

 

Iowa State course, properties of light (sort of just formulas),

http://avogadro.chem.iastate.edu/CHEM513/513-1.pdf

physicaloptics

http://avogadro.chem.iastate.edu/CHEM513/513-2.pdf

            http://avogadro.chem.iastate.edu/CHEM513/513-3.pdf

Optical fiber tutorial from PTI-OBB

            http://www.pti-nj.com/obb_fibers.html

 

Optics companies: (see above first)

Edmund Optics

http://www.edmundoptics.com/onlinecatalog/browse.cfm

Edmund Scientific, WIDE VARIETY OF LENSES AND MIRRORS, originally for astronomy hobbyist

http://scientificsonline.com/category.asp_Q_c_E_424411

American Science Surplus Center—great source for cheap optics

http://www.sciplus.com/category.cfm?subsection=21

Mark Optics, CA

http://markoptics.com/pages/products.htm

CVI Laser and Optics

http://www.cvilaser.com/PublicPages/Pages/default.aspx