物理科学与技术学院 chapter 5 polarization. 5.1 polarized light and natural light 、 degree...
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物理科学与技术学院
Chapter 5
Polarization
5.1 polarized light and natural light 、 degree of polarization 偏振光与自然光、偏振度5.2 polarization by reflection and refraction 、 Brewster’s law 由反射和折射获得偏振光 布儒斯特定律5.3 double refraction in uniaxial crystal 单轴晶体的双折射现象 5.4 Huygen’s explanation of double refraction by wavefront 用波面的概念解释双折射现象5.5 polarization prism and analyser Malus law 偏振棱镜和偏振片 马吕斯定律5.6 elliptically and circularly polarized light wave plate 椭圆偏振光与圆偏振光 波片
5.8 detection of the state of polarization 偏振态的实验检验5.9 interference of polarized light 偏振光的干涉
5.10 photoelastic effect and electro-optical effect 光弹性效应和电光效应5.11 rotation of the plane of linearly polarized light 线偏振光沿晶体光轴传播时振动面的旋转
5.1 polarized light and natural light 、degree of polarization
transverse wave 横波 —the light is propagated as transverse.
longitudinal wave 纵波
波的振动方向对传播方向具有对称性。
波的振动方向对传播方向没有对称性 偏振。
5.1.1 polarization and polarized lightaccording to frequency:
monochromatic 单色光
nonmonochromatic 复色光{E
在垂直于光传播方向的平面内光矢量的振动状态。
—the light is propagated as longitudinal.
electric vector
optical vector光矢量
state of polarization 偏振态— state of the vibration on the propagation of light.
Pre
fac
e
Monochromatic light is used to discuss the state of polarization
natural lightunpolarized
自然光
circularly polarized light圆偏振光
elliptically polarized light椭圆偏振光
right handed 右旋
sort of state of polarization 偏振态的分类
partial polarized light 部分偏振光
polarized light完全偏振光
linearly polarized light平面偏振光 ( 线偏振光 )
left handed 左旋
right handed 右旋
left handed 左旋
5.1.2 natural light and polarized light 自然光与偏振光
E ·
light travels towards to you
EEy
Ex
y
x
sinEE y
1. linearly polarized light 平面偏振光 ( 线偏振光 )
cosEEx
· · · ··
krtAE cos
resolve into two component
vibrations are perpendicular to plane of paper vibrations are parallel to plane of paper
2.natural light 自然光
yx EE xyx IIII 2
resolvent
a natural beam can be resolved into two incoherent components ,which are perpendicular to each other with equal magnitude
·· ·
incoherent
5.1.3 partially polarized light and degree of polarization
polarized+unpolarized
最常讨论的部分偏振光可看成是自然光和线偏振光的混合,
resolve
incoherent
·· ·· ·· ··
天空的散射光和水面的反射光就是这种部分偏振光,它可以分解如下:
degree of polarization 偏振度
minmax
minmax
IIII
Pdegree of
polarization
unpolarized P = 0
polarized P = 1
partially polarized 0<P<1
5.2.1 Brewster’s angle 布儒斯特角
221
iiwhen rp=0 polarized, have no parallel component
write as i10 i10——Brewster’s angle
22101 sinsin inin 102101 cossin inin
1
210tan
nn
i
unpolarizedpartial polarized
5.2.2 linearly polarized light by refraction 由折射获得偏振光 transmitted light is polarized ,the vibration being in plane of incidence
Laser-tube cavity激光器谐振腔
Brewster window 布儒斯特窗
a pile of glass plates 玻璃堆
5.2 polarization by reflection and refraction 、 Brewster’s law
unpolarized beam is not incident at Brewster’s angle incident with :
21
21
21
21
21
21
21
21'
cos
cos
cos
cos
sin
sin
tan
tan
1
1
ii
iir
ii
ii
ii
ii
ii
ii
A
Ar
s
p
pp
1
21
21
ii
ii
cos
cos
''
11 spsp AArr
11 sp AA
Reflected and refracted natural light are partially polarized light 自然光反射和折射后成为部分偏振光
·
···
· · ·n1
n2
i1 i1'
i2
·· S
P
5.2.3 explanation of polarization by reflection and refraction
书 P.206 例 5-1自然光以入射角 i 投射到水面上,使发射光成为完全偏振光。现有一块玻璃浸于水中,如光从玻璃面反射也为完全偏振光,试求水面与玻璃面之间的夹角。解:
33.1
1tan 1
水
空气
n
ni 0265361 i
9010 ii
65921112 ii
33.1
5.1tan 2
水
玻
n
ni 6162482 i
5.3 double refraction in uniaxial crystal
5.3.1 ordinary ray and extraordinary ray
2.ordinary ray and extraordinary ray寻常 (o) 光和非寻常 (e) 光
a ray of light is refracted by a crystal, it gives two refracted rays自然光入射到各向异性介质中,折射光分成两束的现象。
1. double refraction in1
n2
ro
reanisotropic
unpolarized
o e
o ornin sinsin 21 O ray is at plane of incidence
{
e E ray is not always at plane of incidence
.constsin
sin
er
i
{
obey laws of refraction 遵从折射定律
usually,not obey laws ofrefraction 一般不遵从折射定律
· · · calcite 方解石o
ee
o· · ·rotate calcite round the incident ray as an axis
calcite方解石
偏振片
vibrations of two refracted rays are perpendicular to each other双折射的两束光振动方向相互垂直
象折射现双折射现calcite
Phenomenon of double refraction
光光双折射
纸面纸面
光光双折射
纸面纸面
光光双折射
纸面纸面
光光双折射
纸面纸面
光光
paperpaper
image by o ray
image by E ray
when calcite is rotated,image of o ray remains stationary o 光的像不动,
image of e ray rotates with the rotation of crystal 光的像围绕 o 光的像旋转
calcite
5.3.2 optic axis 光轴
a direction, not a line ,along which the double refraction is a
bsent 特定的方向,晶体中光沿这个方向传播时,不发生双折射现象。
Crystallised CaCO3(Iceland spar)方解石晶体(冰洲石)
A
B
102° 78°
1. optic axis 光轴
propagation along optic axis n()=no
propagation perpendicular to optic axis n()=ne
{optic axis
Extraordinary ray
uniaxial crystal 单轴晶体: calcite 方解石、 quartz 石英
biaxial crystal 双轴晶体:云毋、 sulfur 硫磺、 topaz 黄玉{5.3.3 principal section 主截面
晶体光轴与晶体表面法线构成的平面叫主截面
a plane , which contains the optic axis and thenormal of the crystal face, is called principal section
A
B
102° 78°
optic axis
normal
for every point there are three principal section
note the difference from the definition in Chinese textbook
P.207
o rayoptic axis
principal plane of
o ray
· · ··e ray
optic axis
principal plane of e ray
o 光的振动方向垂直于垂直于 o 光的主平面
e 光的振动方向平行于平行于 e 光的主平面 usually, vibrations of o ray and e ray are not perpendicular to each other
vibration of o ray is perpendicular to its principal plane
vibration of e ray is parallel to its principal plane
principal plane 主平面a plane , which contains the optic axis and the rayof light, is called principal plane
principal plane of the ordinary ray
principal plane of the extraordinary ray
optic axis in the plane of incidencethe principal planes of o ray and e ray coincidevibrations of o ray and e ray are perpendicular to each other
commentscomments : : general, the angle between two principal planes is general, the angle between two principal planes is very small, the vibrations of o ray and e ray are almost normalvery small, the vibrations of o ray and e ray are almost normal
5.3.4 relative intensity of o ray and e ray o 光与 e 光的相对光强
a. incidence of natural light
optic axis
··
·
·
·
e
calcite
·
o
I
2,
222 I
AI
A eo
2I
II eo
special case: normal incidence
special case:
principal section
cos
sin
AA
AA
e
o
2tane
o
I
I
b.incidence of linearly polarized light
Ae
Ao θ
rotating the crystal round incident ray introduces the rotation of principal section θ changes
θ =0 , I0=0, Ie=Iθ =90 , I0=I ,Ie=0
in crystal the wavefront of o ray is spherical o 光波面是球面
in crystal the wavefront of e ray is an ellipsoid of revolution e 光波面是旋转椭球面
x
z
x
z
rrn
zen
xon o
o nc
v
ee n
cv
rn varies with the different vibration direction velocity of light varies
n
cv
uniaxial :symmetry of revolution around optic axis
vibration is normal to z:
vibration is parallel to z:
nc
v 'other direction vibration n between on en~
varies with the direction in crystal
5.4 Huygen’s explanation of double refraction by wavefront
Opic axis
principal plane----contains the optic axis and the ray of light
o ray----vibration is normal to principal plane
at any direction,vibration is normal to optic axis
oo n
cv wavefront is spherical——
e ray----vibration is parallel to principal plane
vibration is normal to z
ee n
cv vibration is parallel to z
oo n
cv
wavefront is an ellipsoid of revolution——
propagation along zpropagation along z
propagation is propagation is normal to znormal to z
o ray has same velocity at any direction
e ray has different velocity at different direction
positive crystal 正晶体negative crystal 负晶体
ve<vo
ve>vo
quartz 石英calcite 方解石{
5.4.2propagation direction of o ray and e ray in uniaxial crystal
a. optic axis in the plane of incidence, oblique incidence
r0
i····
voΔt
veΔt
cΔto
oo
nci
r
vsin
sinA···
·B
D
e o re
··
optic axis
··
b. optic axis is normal to the surface, normal incidence
c. optic axis is parallel to the surface, normal incidence
e e·· ··· ·
光轴 晶体
··
o o
·· ··· ··
···
no doublerefractionoptic axis
no separation
same velocity
double refraction happens
no separation but different velocity
d. optic axis is normal to the plane of incidence,normal incidence
· ·optic axis • • •
··
••
••
o oe e
double refraction happens
same as “c ”case
optic axis • • • o
e
••
e. optic axis is normal to the plane of incidence, oblique incidence
5.5 polarization prism and analyser Malus law
1 .Nicol prism 尼科耳棱镜
•• ••
••
no=1.658ne=1.486nb=1.550e
2.Wollaston prism 渥拉斯顿棱镜
• •• •
Canada balsam加拿大树胶
• • • •••
•e
o
tansin2 1eo nn
e
o
5.5.1 polarization prism 偏振棱镜
• •• •
• •
• •• •
• • • •••
•e
o
glass
examples:
( 1 )
( 2 )
Calcite(negative crystal)
no=1.658ne=1.486
no=1.658ne=1.486nglass=1.5
calcite
• •••
•e
o
5.5.2 analyser (polarization plate)
5.5.3 Malus law 马吕斯定律
P2
A1
P2
A 2= A1cos
Malus law 马吕斯定律 (1809)
2 2 1 2 cosAI , I
21
02
1 1 AI
202 cos
2I
I
—— extinguishintensity vanishes 消光
2/0 0max2 III ,
02 2 I,
linear IP1
plane of transmission
natural light I0
· ··
例 5-2 假定在两个静止的、理想的、正交的起偏器之间有另一个理想的起偏器以角速度 w 旋转,试证透射光的强度满足下列关系式: tI
I 4cos181
★ 例 5-3 设一水晶棱镜的顶角 A 为 60 度,光轴与棱镜主截面垂直,钠光以最小偏向角的方向在棱镜中折射,用焦距为0.5m 的透镜聚焦, no=1.54425,ne=1.5536, 试求 o 光和 e 光两谱线的间隔为多少?
5.6 elliptically and circularly polarized light wave plate
circularly polarized 圆偏振光—— tip of the vector draws a circle
elliptically polarized 椭圆偏振—— tip of the vector draws a ellipse{face to the ray
clockwise——right handed 右旋
counter-clockwise——left handed 左旋{
5.6.1 description of elliptically and circularly polarized light 圆偏振光和椭圆偏振光的描述
b.theory
a.definition
elliptically polarized light consists of two plane polarized rayswith same frequency, orthogonal vibrations, traveling along same direction
椭圆偏振光可通过两列频率相同,振动方向相互垂直, 沿同一方向传播的线偏振光叠加得到。
kztAE
kztAE
yy
xx
cos
cosamplitude
22
2
2
2
sincos2y
y
x
x
y
y
x
x
A
E
AE
A
E
AE
=0 ,
= /2
= 其他值
y
y
x
x
A
E
AE
12
2
2
2
y
y
x
x
A
E
AEdiscussion
linear polarized
AxAy elliptically polarized
Ax=Ay circularly polarized
oblique elliptically polarized
{
圆偏振光可通过两频率相同,振动方向相互垂直,且振幅相同, 位相差 (2k+1)/2, 沿同一方向传播的线偏振光叠加得到。
circularly polarized light consists of two plane polarized rayswith same frequency, orthogonal vibrations of equal amplitude, phase difference of (2k+1)/2 ,traveling along same direction
5.6.2 wave plate 波(晶)片wave plate——a plate of doubly refracting uniaxial crystal,which optic axis is parallel to the surface. o ray and e ray travel along same direction with different velocities
d—thickness of plate
nod——optical path of o ray
ned——optical path of e ray
= ( no- ne ) dphase difference:
¼ 波片 dnn eo 2
122
12
k
k
½ 波片
principal section
optical path difference:
quarter wave plate
half wave plate(半波片 )
incident linearly polarized light makes an angle of with optic axispassing a half wave plate , the emergent light is still a linearly polarized light,which direction of polarization is rotated by 2
b.plane polarized light is incident
intensity ratio of o ray and e ray : sin2/cos2
phase difference : dnn eo 2
e 光
o 光
a. natural light is incident
two components of incident light have unfixed phase difference o and e rays have unfixed phase difference emergent light is natural light
for half wave plate:
A
Ao
Ae
Ao'
2optic axis
y
d
xA
Ao
Ae
linear
when the ray have traveled through the thickness d in crystal, a phase difference is introducted between o 、 e rays:
A
Ao
Ae
optic axis P
elliptically
general case----- product an elliptically polarized light
d optic axis
wave plate
5.6.3 production of elliptically and circularly polarized light 圆偏振光和椭圆偏振光的产生
sinAAo cosAAe
2
dnn eo
a. linearly polarized light passes through a wave plate
and),( eo AA 4
2
3,
2
b. linearly polarized light passes through a quarter wave plate
4
dnn oe
4
circularly polarized light
2,0 plane polarized light
thickness of the wave plate2
240
,, elliptically polarized light(normal)
product an circularly polarized light
special case -----
c. production of elliptically and circularly polarized light from natural light
incidence of natural lighttransmitted rays have no fixed phase difference-----natural light
at first, the natural light must pass a polarizer to become a linearly polarized light
Pnatural light I0
· ··
optic axis
quarter wave plate when =45°
circularly polarized
usually, elliptically polarized light
例 5-4 一束圆偏振光,( 1 )垂直入射到 1/4 波片上,求透射光的偏振态;( 2 )垂直入射到 1/6 波片上,求透射光的偏振态;
例 5-5 一单色自然光通过尼科尔棱镜 N1 , N2 和晶片 C ,其次序如图示, N1 的主截面水平, C 对应于这波长的 1/4 波片,其主截面与竖直方向成 30 度,试问:( 1 )在 N1 和 C 之间, C 和 N2 之间,以及从 N2 透射出来的光各是什么性质的光?( 2 )若入射光的强度为 I0 ,则上述各部分的光的强度各是多少? 注 : 此例最好放到偏振光干涉之后讲
Calculate the thickness of (i) a quarter wave plate and (ii) a half wave plate given that
nmnn oe ,544.1,553.1
5.7 detection of the state of polarization 偏振态的实验检验
5.7.1 Compensator
Babinet’s Compensator
Soleil’s Compensator
· ·· ·
· ·· ·
5.7.2 detection of the state of polarization
incident light
incident on a rotating polarizer
intensity changes and vanishes
intensity does not change
intensity changes but never vanishes
plane polarized either circularly polarized or unpolarized
either ellipticallypolarized or partially polarized
result result result
case 2 case 3case 1
case 2: original beam
incident on a rotating polarizer
intensity changes and vanishes
intensity does not vanish
plane polarized
either circularlypolarized or unpolarized
result result
incident on a quarter wave plate
unpolarized
unpolarized
circularly polarized
case 3: original beam
incident on a rotating polarizer
intensity changes and vanishes
intensity does not vanich
plane polarized
either elliptically polarized or partially polarized
result result
incident on a quarter wave plate,whose optic axis is parallel to max
partially polarized(linearly polarize +natural)
partially polarized
circularly polarized
▲ 如何区分由自然光和椭圆偏振光组成的 部分偏振光与由自然光和线偏振光组成 的部分偏振光?
思考
▲ 如何区分由自然光和圆偏振光组成的部分 偏振光与自然光?
5.8 interference of polarized light 偏振光的干涉
5.8.1 set up and intensity distribution 偏振光干涉装置和强度分布
natural light
polarizerP1
d
wave plate C
optic axis
A1o
A2o
P2
P1 CA1 A1e
A2e
after P1 :
polarizerP2
interference
sin11 AA o cos11 AA e
sinsinsin 112 AAA oo
coscoscos 112 AAA ee
after P2 :
Interference intensity :
2'
sin2sin2sincos
'coscossincossin2
coscossinsin
'cos2
2221
21
2221
2221
2222
22
A
A
AA
AAAAI eoeo
dnn eo 2
phase difference :
' =——P1 , P2 are at same side of optic axis
+ ——P1 , P2 are at opposite side of optic axis{
—destructive interference
if d is various , there are equal thickness fringes in screen
),2,1(,2
122
knn
kdk
oe
oe nn
kdk
)12(
P1 , P2 are at opposite side of optic axis:
),2,1(,2
122
knn
kdk
oe
,...)2,1,0(,)12(
knn
kdk
oe
—constructive interference
P1 , P2 are at same side of optic axis:
—constructive interference
—destructive interference
especially :
( 1 ) P1 // P2 ,
( 2 ) P1 P2 ,
2
2sin2sin1 222
1//
AI
2sin2sin
2sin2sin2sin
2221
22221
A
AI
P1 , P2 are at opposite side of optic axis
21// AII
incidence of monochromatic light 单色光入射fixed A1
2,
dnn eo 2
phase difference :
equal thickness: I is related to
unequal thickness: I is related to and d{intensity I is only related to ,
5.8.2 incidence of white light白光入射 is related tocolor fringes
(显)色偏振
if the thickness of wave plate is uniform, the screen presents coloured ------complementary colour 互补色 of destructive interference at a wavelength. It is called chromatic polarization
end