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Medical Engineering & Physics
jou rn al h om epage: www.elsevier.com/locate/medengphy
Nonstationary multivariate modeling of cerebral autoregulation
during hypercapnia
Kyriaki Kostoglou
a
, Chantel T. Debert
b
, Marc J. Poulin
c,d,e,f,g
, Georgios D. Mitsis
a,∗
a
Department of Electrical and Computer Engineering, University of Cyprus, Nicosia, Cyprus
b
Department of Physical Medicine and Rehabilitation, Faculty of Medicine, University of Calgary, AB, Canada
c
Department of Physiology & Pharmacology, Faculty of Medicine, University of Calgary, AB, Canada
d
Department of Clinical Neurosciences, Faculty of Medicine, University of Calgary, AB, Canada
e
Faculty of Kinesiology, University of Calgary, AB, Canada
f
Hotchkiss Brain Institute, Faculty of Medicine, University of Calgary, AB, Canada
g
Libin Cardiovascular Institute of Alberta, Faculty of Medicine, University of Calgary, AB, Canada
a r t i c l e i n f o
Article history:
Received 5 March 2013
Received in revised form 7 September 2013
Accepted 13 October 2013
Keywords:
Cerebral hemodynamics
Time varying systems
CO2 reactivity
Laguerre functions
Recursive Least Squares
Multiple forgetting factors
a b s t r a c t
We examined the time-varying characteristics of cerebral autoregulation and hemodynamics during a
step hypercapnic stimulus by using recursively estimated multivariate (two-input) models which quan-
tify the dynamic effects of mean arterial blood pressure (ABP) and end-tidal CO
2
tension (P
ETCO
2
) on middle
cerebral artery blood flow velocity (CBFV). Beat-to-beat values of ABP and CBFV, as well as breath-to-
breath values of P
ETCO
2
during baseline and sustained euoxic hypercapnia were obtained in 8 female
subjects. The multiple-input, single-output models used were based on the Laguerre expansion tech-
nique, and their parameters were updated using recursive least squares with multiple forgetting factors.
The results reveal the presence of nonstationarities that confirm previously reported effects of hyper-
capnia on autoregulation, i.e. a decrease in the MABP phase lead, and suggest that the incorporation of
P
ETCO
2
as an additional model input yields less time-varying estimates of dynamic pressure autoregulation
obtained from single-input (ABP–CBFV) models.
© 2013 IPEM. Published by Elsevier Ltd. All rights reserved.
1. Introduction
Cerebral autoregulation collectively refers to the ability of the
cerebrovascular bed to maintain a relatively constant cerebral
blood flow (CBF) in response to variations in several physiological
variables. The most important of these variables is arterial blood
pressure (ABP); therefore, the relation between ABP and CBF is
typically used to characterize autoregulation. Accurate quantita-
tive assessment of cerebral autoregulation and, more generally,
hemodynamics, is important in the context of cerebrovascular
disease diagnosis and monitoring [1,2]. Following the advance of
transcranial Doppler ultrasound (TCD), which yields accurate mea-
surements of CBF velocity (CBFV) [3], it is now well established that
autoregulation is a dynamic, frequency-dependent phenomenon
[4–6]. Dynamic autoregulation may be assessed from the CBFV
response to step-like, externally induced ABP stimuli or from
spontaneous physiological variability, as the latter exhibits suffi-
ciently broadband characteristics. The majority of the studies that
have assessed dynamic cerebral autoregulation from spontaneous
∗
Corresponding author.
E-mail address: mitsis.georgios@ucy.ac.cy (G.D. Mitsis).
variability have utilized univariate, linear techniques such as
transfer function analysis [4]. However, in this latter study and
other studies, low coherence values (<0.5) between spontaneous
ABP and CBFV fluctuations in the frequency range below 0.07 Hz
have been reported. Since coherence is a measure of linearity in
the dynamic relation between ABP and CBFV, this suggests that
nonlinearities and/or other physiological variables may have an
important effect in this frequency range. In this context, it is well
known that the cerebral vasculature is extremely sensitive to arte-
rial CO
2
changes; for instance, spontaneous variations of end-tidal
CO
2
(P
ETCO
2
) have been shown to influence CBFV as well as the
BOLD fMRI signal [7,8]. Therefore, multivariate models of cerebral
hemodynamics incorporating CO
2
as an additional input have been
proposed in order to characterize autoregulation [7,9]. The pres-
ence of nonlinearities has been also suggested [5,6], corroborating
that the aforementioned low coherence between ABP and CBFV is
due to both factors. In our previous studies, we have demonstrated
that both dynamic nonlinearities and CO
2
variability account
for a significant fraction of the low-frequency CBFV variability
during resting conditions, orthostatic stress as well as ganglion
blockade [7,10,11]. Collectively, these findings suggest that multi-
variate and/or nonlinear modeling approaches yield more accurate
quantitative descriptions of cerebral hemodynamics below 0.07 Hz.
1350-4533/$ – see front matter © 2013 IPEM. Published by Elsevier Ltd. All rights reserved.
http://dx.doi.org/10.1016/j.medengphy.2013.10.011