Chapter 8 measurement and theory, 1 basics, Chapter 8 – INFICON STM-2 USB Thin Film Rate/Thickness Monitor User Manual

Page 91

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STM-2 Operating Manual

Chapter 8

Measurement and Theory

8.1 Basics

The Quartz Crystal deposition Monitor (QCM) utilizes the piezoelectric sensitivity
of a quartz monitor crystal to added mass. The QCM uses this mass sensitivity to
control the deposition rate and final thickness of a vacuum deposition.

When a voltage is applied across the faces of a properly shaped piezoelectric
crystal, the crystal is distorted and changes shape in proportion to the applied
voltage. At certain discrete frequencies of applied voltage, a condition of sharp
electro-mechanical resonance is encountered.

When mass is added to the face of a resonating quartz crystal, the frequency of
these resonances are reduced. This change in frequency is very repeatable and is
precisely understood for specific oscillating modes of quartz. This heuristically
easy-to-understand phenomenon is the basis of an indispensable measurement
and process control tool that can easily detect the addition of less than an atomic
layer of an adhered foreign material.

In the late 1950’s it was noted by Sauerbrey

1,2

and Lostis

3

that the change in

frequency, DF = F

q

-F

c

, of a quartz crystal with coated (or composite) and uncoated

frequencies, F

c

and F

q

respectively, is related to the change in mass from the

added material, M

f

, as follows:

[1]

where M

q

is the mass of the uncoated quartz crystal. Simple substitutions led to the

equation that was used with the first “frequency measurement” instruments:

[2]

where the film thickness, T

f

, is proportional (through K) to the frequency change,

DF, and inversely proportional to the density of the film, d

f

. The constant, K =

N

at

d

q

/F

q

2

; where d

q

(= 2.649 g/cm

3

) is the density of single crystal quartz and N

at

(=166100 Hz cm) is the frequency constant of AT cut quartz.

1.G. Z. Sauerbrey, Phys. Verhand .8, 193 (1957)
2.G. Z. Sauerbrey, Z. Phys. 155,206 (1959)
3.P. Lostis, Rev. Opt. 38,1 (1959)

M

f

M

q

-------

F

F

q

-----------

=

T

f

K F

d

f

----------------

=

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