B s c I e n t I f I c ® e X p e r I m e n t s g o I n g o n e s t e p f u r t h e r M1 bs1 p (45°) M2 bs2 laser a (45°) laser p1 P2 (0°) (90°) laser mach-Zehnder interferoMeter


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UE4030520 EN



2
3 B S c i e n t i f i c ® E x p e r i m e n t s
. . . g o i n g o n e s t e p f u r t h e r
M1
BS1
2
1
P
(45°)
M2
BS2
LASER
2
1
A
(45°)
LASER
2
1
P1
P2
(0°)
(90°)
LASER
Mach-Zehnder interferoMeter
OP T IC S / WAV E OP T IC S
OBJECTIVE
Demonstration of “quantum erasure” in an experiment by analogy.
Ue4030520
BASIC PRINCIPL ES
Light itself can be described in quantum mechanics by means of wave equations. From this it is 
possible to derive the spatial distribution of the probability density in the form of the square of 
the modulus of the wave function. The combination of two beams corresponds to superposition 
of two wave functions. The probability density then contains a mixed term which describes the 
interference pattern. Light is therefore suitable for experiments which demonstrate quantum 
mechanical phenomena by analogy.
Ue4030520
SUMM A RY
Light itself can be described in quantum mechanics by means of wave equations. From this it is pos-
sible to derive the spatial distribution of the probability density in the form of the square of the 
modulus of the wave function. Light is therefore suitable for experiments which demonstrate quantum 
mechanical phenomena by analogy. Such an analogy experiment demonstrates the so-called quantum 
eraser effect by setting up a Mach-Zehnder interferometer and observing interference between the 
split beams on a screen. If two perpendicular polarisers are placed in the paths of the split beams, the 
interference vanishes since, in quantum mechanical terms, it is possible to determine the path a pho-
ton has taken. If a third polarising filter set at an angle of 45° is placed directly in front of the screen, 
this quantum information is “erased” and the interference can be seen once again.
E X PERIMEN T 
PROCEDURE

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