Biomedical Engineering Reference
In-Depth Information
high temporal resolution, or in measurement of vascular transit-
time maps associated with diagnosis of cerebrovascular diseases, it
would be essential to determine CBF dynamically. One efficient
way to accomplish dynamic measurements of CBF with ASL is to
impose a systematic and periodic variation of the degree of label-
ing
α
( t ). According to Equation (13.4) , periodic variations in
α
( t ) would cause periodic variations in the tissue magnetization,
and a temporal analysis of the tissue response would yield dynamic
quantification of T 1 b ,
and CBF. This transient analysis has been
named dynamic ASL (DASL) (53, 65) .
The dynamic analysis can be introduced by simply allowing
the degree of labeling
τ
( t )in Equation (13.5) to be a time-
dependent, periodic function. In such case, Equation (13.5) can
be integrated characterizing the time evolution after steady-state
has been reached of a system subject to a specific time-varying
labeling function, and is given by (65) :
α
e ( t τ ) T 1 app
CBF
λ
M b
( t ) M b
e τ / T 1 a
M b ( t )
=
2
α
(13.8)
where
denotes the convolution product. From Equation
(13.8) , it is important to note that independent of the labeling
function, the tissue response has a time shift introduced by the
transit time
.
In theory, the labeling function may be arbitrarily defined as
long as the arterial spins can be inverted accordingly, so that defi-
nition of the labeling function should be determined by the exper-
imental goals. For example, the use of a periodic square labeling
function of period 2
τ
defined as follows:
e τ/ T 1 a
α 0 ·
,
0
<
t
α
( t )
=
(13.9)
0
,
<
t
2
will
produce
a
periodic
tissue
magnetization
response,
given by (65) :
1
α 0 e τ / T 1 a CBF
λ
M b
M b (
τ<
t
+ τ
)
=
2 T 1 app
1
e T 1 app e ( t τ ) T 1 app
e T 1 app
e ( t τ ) T 1 app
1
×
+
e T 1 app
1
2 T 1 app α 0 e τ / T 1 a CBF
λ
M b
M b (
+ τ<
t
2
+ τ
)
=
1
e T 1 app e T 1 app
e T 1 app
e T 1 app
e ( t τ ) T 1 app
1
×
+
e T 1 app
(13.10)
 
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