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Am J Physiol Heart Circ Physiol 279: H2558-H2567, 2000;
0363-6135/00 $5.00
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Vol. 279, Issue 5, H2558-H2567, November 2000

SPECIAL COMMUNICATION
Assessing baroreflex gain from spontaneous variability in conscious dogs: role of causality and respiration

A. Porta1, G. Baselli2, O. Rimoldi3, A. Malliani1,3, and M. Pagani1,4

1 Dipartimento di Scienze Precliniche, Laboratorio Interdisciplinare Tecnologie Avanzate di Vialba, 3 Centro Ricerche Cardiovascolari, Consiglio Nazionale della Ricerca, Medicina Interna II, and 4 Medicina Interna I, Ospedale L. Sacco, Universitá degli Studi di Milano, 20157 Milan; and 2 Dipartimento di Bioingegneria, Politecnico di Milano, 20133 Milan, Italy


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
CAUSAL PARAMETRIC MODELING...
TRADITIONAL APPROACHES TO...
METHODS
RESULTS
DISCUSSION
APPENDIX
REFERENCES

A double exogenous autoregressive (XXAR) causal parametric model was used to estimate the baroreflex gain (alpha XXAR) from spontaneous R-R interval and systolic arterial pressure (SAP) variabilities in conscious dogs. This model takes into account 1) effects of current and past SAP variations on the R-R interval (i.e., baroreflex-mediated influences), 2) specific perturbations affecting R-R interval independently of baroreflex circuit (e.g., rhythmic neural inputs modulating R-R interval independently of SAP at frequencies slower than respiration), and 3) influences of respiration-related sources acting independently of baroreflex pathway (e.g., rhythmic neural inputs modulating R-R interval independently of SAP at respiratory rate, including the effect of stimulation of low-pressure receptors). Under control conditions, alpha XXAR = 14.7 ± 7.2 ms/mmHg. It decreases after nitroglycerine infusion and coronary artery occlusion, even though the decrease is significant only after nitroglycerine, and it is completely abolished by total arterial baroreceptor denervation. Moreover, alpha XXAR is comparable to or significantly smaller than (depending on the experimental condition) the baroreflex gains derived from sequence, power spectrum [at low frequency (LF) and high frequency (HF)], and cross-spectrum (at LF and HF) analyses and from less complex causal parametric models, thus demonstrating that simpler estimates may be biased by the contemporaneous presence of regulatory mechanisms other than baroreflex mechanisms.

cardiovascular variability; linear parametric modeling; identification techniques


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
CAUSAL PARAMETRIC MODELING...
TRADITIONAL APPROACHES TO...
METHODS
RESULTS
DISCUSSION
APPENDIX
REFERENCES

EVALUATION OF THE BAROREFLEX GAIN is considered an important tool in clinical practice (16). The baroreflex gain is usually estimated by inducing an increase of arterial pressure by means of a vasoconstrictive drug and by evaluating the subsequent lengthening of the heart period (23). Because this procedure is based on a nonphysiological stimulus that may alter the actual value of the baroreflex gain, several techniques have been proposed to evaluate the baroreflex gain based on the spontaneous variability of systolic arterial pressure (SAP) and heart period (R-R interval). Traditional methods are based on 1) detection of sequences of SAP and R-R interval values characterized by the simultaneous increase or decrease of both variables (10), 2) calculation of the power spectrum of R-R interval and SAP variability series (19), and 3) calculation of the magnitude of the SAP-R-R transfer function (22).

The main limitation of these methods is that they are not capable of evaluating the fraction of R-R interval variability driven by SAP changes because they do not impose causality (i.e., a relationship linking the current R-R interval to past SAP values). Therefore, they cannot reveal whether the observed changes in SAP and R-R interval are the result of feedback mechanisms from SAP to R-R interval (i.e., the baroreflex pathway) or of the feedforward relationship from R-R interval to SAP (mainly related to Starling and windkessel effects). As a consequence, these methods can only produce indexes lumping together the properties of both paths, and denervation experiments or pacing are required to disentangle the feedback pathway from the feedforward pathway (2, 17). Moreover, the effects of other variables on the estimate of the baroreflex gain are not explicitly taken into account, although they are acknowledged. For example, Smyth et al. (23) suggested fixing the respiratory phase in assessing the baroreflex gain. Changes of the R-R interval synchronous with respiration can occur independently of variations in SAP and, therefore, of the arterial baroreflex circuit. For example, changes in venous return and central venous pressure related to respiration can produce activation or deactivation of the low-pressure receptors (25) and, therefore, through the Bainbridge reflex, changes in the heart period (28). Moreover, even effects of centrally mediated rhythmic variations in the autonomic drive to the sinus node (14) produce a certain amount of R-R variability not mediated by the baroreceptive circuit. The presence of a fraction of R-R interval variability independent of SAP changes, if not explicitly addressed, may lead to an overestimate of the baroreflex gain.

The aim of this study is to propose a model-based approach to the evaluation of the baroreflex gain capable of imposing causality (i.e., to evaluate the fraction of R-R variability driven by SAP changes) and directly accounting for sources capable of influencing the R-R interval independently of SAP changes (mainly the effects of slow rhythms and respiration directly driving R-R interval).

Three parametric linear model structures are considered: 1) the R-R-SAP exogenous model (X model), 2) the R-R-SAP exogenous model with autoregressive (AR) input (XAR model), and 3) the R-R-SAP exogenous model with exogenous respiration and AR input (XXAR model). In the X model the R-R interval depends on the current and several previous SAP values. In the XAR model the R-R-SAP relationship is described by an X model, but rhythmic sources affecting R-R interval independently of baroreflex pathway are also modeled. In the XXAR model, in addition to XAR features, the nonbaroreflex effects of respiration on R-R interval are described.

Comparison of the baroreflex gain estimated by the X model with those derived from traditional methods (10, 19, 22) allows us to clarify the role of causality in the estimation of baroreflex gain. Comparison of the baroreflex gains obtained by the proposed parametric models allows us to evaluate the distorting effects of sources driving R-R interval variability independently of SAP changes on the estimate of the baroreflex gain and to propose a model (i.e., the XXAR model) providing a less biased estimate of the baroreflex gain.

The study was carried out on conscious dogs (21) undergoing the following experimental conditions: 1) control, 2) nitroglycerine infusion (NT) producing a sympathetic activation by decreasing SAP, 3) coronary artery occlusion (CAO) increasing sympathetic activity without an important change in mean arterial pressure, and 4) total arterial baroreceptive denervation (TABD) preventing SAP changes to produce baroreflex-mediated R-R interval variations.


    CAUSAL PARAMETRIC MODELING APPROACH TO ESTIMATE OF BAROREFLEX GAIN
TOP
ABSTRACT
INTRODUCTION
CAUSAL PARAMETRIC MODELING...
TRADITIONAL APPROACHES TO...
METHODS
RESULTS
DISCUSSION
APPENDIX
REFERENCES

This section describes the three parametric models (X, XAR, and XXAR) capable of extracting the baroreflex gain from spontaneous variability of R-R interval and SAP.

The main characteristics of these models are that 1) they describe the linear relationship among changes of the variables around a set point (the mean value); 2) they are dynamic because several past samples are considered; 3) they are causal because they fix a temporal direction of the influences (R-R interval changes depend on current and past variations of SAP); and 4) they are defined in the beat-to-beat domain, thus allowing us to reduce the complexity of the model structure (we do not have to reconstruct all the features of the waveform) while maintaining information about the short-term regulatory mechanisms (6, 11).

In the discussion of the three models rri, sapi, and respi represent the difference between the actual sample RRi, SAPi, and Respi and their mean values, where RR is R-R interval, Resp is the respiratory signal, and i is the progressive cardiac beat number.

R-R-SAP X model. The simplest parametric model describing the rr series and the causal influences of sap on rr can be defined as
rr<SUB><IT>i</IT></SUB><IT>=</IT><LIM><OP>∑</OP><LL><IT>k=0</IT></LL><UL><IT>p</IT></UL></LIM><IT> h</IT><SUB>rr<IT>−</IT>sap,<IT>k</IT></SUB><IT>·</IT>sap<SUB><IT>i−k</IT></SUB><IT>+w</IT><SUB>rr,<IT>i</IT></SUB> (1)
where hrr-sap,k is the kth coefficient setting the influences of sap on rr and wrr is a zero mean white noise with variance lambda wrr2. Therefore, the rri value depends on the sap (the exogenous signal) at the same cardiac beat (i.e., sapi) and on p past values of sap. In this way, causal effects of SAP on R-R interval (i.e., the baroreflex-mediated influences) are explicitly addressed. Fig. 1A represents this relationship in terms of a block diagram. All the rr variability independent of sap is lumped into wrr. The sap series is modeled as an AR process of order p
sap<SUB><IT>i</IT></SUB><IT>=</IT><LIM><OP>∑</OP><LL><IT>k=1</IT></LL><UL><IT>p</IT></UL></LIM><IT> h</IT><SUB>sap<IT>−</IT>sap,<IT>k</IT></SUB><IT>·</IT>sap<SUB><IT>i−k</IT></SUB><IT>+w</IT><SUB>sap,<IT>i</IT></SUB> (2)
where hsap-sap,k is the kth coefficient of the AR model and wsap is a zero mean white noise with variance lambda wsap2.


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Fig. 1.   The 3 causal parametric models proposed to describe R-R interval dynamics are shown: exogenous (X) model (A), X with autoregressive (AR) input (XAR) model (B), and XAR with exogenous input (XXAR) model (C). The models differ in describing the effects of inputs affecting R-R interval (rr) independently of systolic arterial pressure (sap). These influences are noise (wrr) without any rhythmic pattern (A), rhythmic patterns (urr) (B), and rhythmic patterns driven by respiration (uresp) and independent of respiration (urr) (C). H, transfer function.

R-R-SAP XAR model. To take into account both direct effects of sap and possible influences (indicated as urr), including rhythmic influences, affecting rr independently of sap, the model described by Eq. 1 can be modified as
rr<SUB><IT>i</IT></SUB><IT>=</IT><LIM><OP>∑</OP><LL><IT>k=0</IT></LL><UL><IT>p</IT></UL></LIM><IT> h</IT><SUB>rr<IT>−</IT>sap,<IT>k</IT></SUB><IT>·</IT>sap<SUB><IT>i−k</IT></SUB><IT>+u</IT><SUB>rr,<IT>i</IT></SUB> (3)
where sap is described as in Eq. 2 and urr is the AR process
u<SUB>rr,<IT>i</IT></SUB><IT>=</IT><LIM><OP>∑</OP><LL><IT>k=1</IT></LL><UL><IT>p</IT></UL></LIM><IT> h</IT><SUB>urr<IT>−</IT>urr,<IT>k</IT></SUB><IT>·u</IT><SUB>rr,<IT>i−k</IT></SUB><IT>+w</IT><SUB>rr,<IT>i</IT></SUB> (4)
where hurr-urr,k is the kth coefficient of the AR model. Therefore, rri depends not only on current and past sap values but also on a source (urr) describing all the influences unrelated to sap but capable of producing rhythmic changes in rr (Fig. 1B). In this way, oscillations generated by mechanisms involving nonbaroreflex circuits (e.g., cardiogenic reflexes mediated by myocardial ischemia) are explicitly addressed.

R-R-SAP XXAR model. The most complex model is introduced to separate the influences of respiration on rr acting independently of sap. It is defined as
rr<SUB><IT>i</IT></SUB><IT>=</IT><LIM><OP>∑</OP><LL><IT>k=0</IT></LL><UL><IT>p</IT></UL></LIM><IT> h</IT><SUB>rr<IT>−</IT>sap,<IT>k</IT></SUB><IT>·</IT>sap<SUB><IT>i−k</IT></SUB><IT>+</IT><LIM><OP>∑</OP><LL><IT>k=0</IT></LL><UL><IT>p</IT></UL></LIM><IT> h</IT><SUB>rr<IT>−</IT>resp,<IT>k</IT></SUB><IT>·</IT>resp<SUB><IT>i−k</IT></SUB><IT>+u</IT><SUB>rr,<IT>i</IT></SUB> (5)
where hrr-resp,k is the kth coefficient setting the influences of resp on rr, and urr is described by Eq. 4. The respiratory signal is modeled as an AR process
resp<SUB><IT>i</IT></SUB><IT>=</IT><LIM><OP>∑</OP><LL><IT>k=1</IT></LL><UL><IT>p</IT></UL></LIM><IT> h</IT><SUB>resp<IT>−</IT>resp,<IT>k</IT></SUB><IT>·</IT>resp<SUB><IT>i−k</IT></SUB><IT>+w</IT><SUB>resp,<IT>i</IT></SUB> (6)
where wresp is zero mean white noise with variance lambda wresp2. Therefore, three inputs are considered to be capable of driving rr changes (Fig. 1C): 1) current and past sap variations producing R-R interval variability via the baroreflex pathway, 2) current and past respiratory changes not mediated by sap variations (e.g., oscillations mediated by respiratory centers and by the activation of low-pressure receptors), and 3) unmeasurable inputs, particularly slow oscillations, independent of sap and resp (e.g., slow rhythms accompanying myocardial ischemia).

Evaluation of baroreflex gain. After the coefficients of the models are identified (see Identification and validation of X, XAR, and XXAR models in the APPENDIX), the block Hrr-sap (Fig. 1) is fed by an artificial signal simulating a unitary ramplike rise of SAP and the slope of the relevant increase of R-R interval is taken as an index of the baroreflex gain. The slope of the R-R interval response is calculated with least-squares linear fitting evaluated on the first 15 samples.

Hypothesis testing and evaluation of performance of model. The adequacy of the model in describing the dynamics of the R-R signal and its interactions with SAP and Resp signals is tested by evaluating whether the residual signals (wrr and wsap for X and XAR models and wrr, wsap, and wresp for the XXAR model) are white and not correlated with each other (see Identification and validation of X, XAR and XXAR models in the APPENDIX).

The performance of the model is evaluated by calculating the goodness of fit (rho ) of the R-R interval series. It is defined as
&rgr;<SUB>rr</SUB><IT>=</IT><FR><NU><IT>&sfgr;</IT><SUP><IT>2</IT></SUP><SUB>rr</SUB><IT>−&lgr;</IT><SUP><IT>2</IT></SUP><SUB><IT>w</IT>rr</SUB></NU><DE><IT>&sfgr;</IT><SUP><IT>2</IT></SUP><SUB>rr</SUB></DE></FR> (7)
where sigma rr2 and lambda wrr2 represent the variance of R-R interval and of its residue, respectively, thus measuring the percent variance of the R-R interval series explained by the proposed model. rho rr = 1 means that the R-R interval power is completely described by the model; an insufficient model structure produces rho rr closer to 0.


    TRADITIONAL APPROACHES TO ESTIMATE OF BAROREFLEX GAIN
TOP
ABSTRACT
INTRODUCTION
CAUSAL PARAMETRIC MODELING...
TRADITIONAL APPROACHES TO...
METHODS
RESULTS
DISCUSSION
APPENDIX
REFERENCES

This section summarizes the most utilized techniques for estimating the baroreflex gain from spontaneous variability series of R-R interval and SAP. These techniques are based on baroreflex sequence (10), power spectrum (19), and transfer function (22) analysis.

Baroreflex sequence analysis. This method is based on the search for sequences characterized by the contemporaneous increase (positive sequence) or decrease (negative sequence) of R-R interval and SAP. The lag (tau ) between R-R interval and SAP samples is chosen as the lag producing the maximum in the normalized R-R-SAP cross-correlation function. Both positive and negative sequences are referred to as baroreflex sequences if they match the following prerequisites: 1) the total of R-R variations is >5 ms; 2) the total of SAP variations is >1 mmHg; and 3) the length of the sequences is four beats (3 variations). For each sequence the slope of the regression line in the plane (SAPi-tau ,RRi) is calculated. All the slopes with correlation coefficient >0.85 are averaged, and this average, represented by alpha BS, has been taken as a measure of the baroreflex gain (10). The reliability of alpha BS depends on the number of baroreflex sequences detected in the series.

Power spectral analysis. The method relies on the calculation of the power spectrum of the rr and sap series (see Power Spectrum Estimate in the APPENDIX) and on the evaluation of the power inside two bands, the low frequency (LF, from 0.04 to 0.14 Hz) and high frequency (HF, ±0.04 Hz around the respiratory rate) bands (26). Two indexes estimating the baroreflex gain are calculated (19) as
&agr;<SUB>PS(LF)</SUB><IT>=</IT><RAD><RCD><FR><NU>P<SUB>rr(LF)</SUB></NU><DE>P<SUB>sap(LF)</SUB></DE></FR></RCD></RAD><IT> &agr;</IT><SUB>PS(HF)</SUB><IT>=</IT><RAD><RCD><FR><NU>P<SUB>rr(HF)</SUB></NU><DE>P<SUB>sap(HF)</SUB></DE></FR></RCD></RAD> (8)
where Prr(LF), Psap(LF), Prr(HF), and Psap(HF) represent the power in LF and HF bands detected on R-R interval and SAP series, respectively. These indexes are reliable if the coherence function (K2) sampled at LF and HF is >0.5 (11), thus meaning that the rr and sap signals are significantly correlated at that specific frequency and, therefore, the power calculated in LF and HF bands is not only the effect of independent noises impinging on both signals.

Transfer function analysis. The R-R-SAP transfer function modulus can be calculated from the zero mean sap and rr series as
‖H<SUB>rr<IT>−</IT>sap</SUB>(<IT>f</IT>)<IT>‖=</IT><FR><NU><IT>‖</IT>C<SUB>rr<IT>−</IT>sap</SUB>(<IT>f</IT>)<IT>‖</IT></NU><DE>P<SUB>sap</SUB>(<IT>f</IT>)</DE></FR> (9)
where Crr-sap is the cross spectrum between rr and sap series and Psap is the spectrum of sap series (see Cross-Spectrum Estimate in the APPENDIX). The transfer function modulus can be sampled at LF and HF detected on sap series (22), thus obtaining two indexes of baroreflex gain that are referred as to alpha CS(LF) and alpha CS(HF). This approach also requires us to test whether K2 is >0.5 at LF and HF (7, 11).


    METHODS
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INTRODUCTION
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TRADITIONAL APPROACHES TO...
METHODS
RESULTS
DISCUSSION
APPENDIX
REFERENCES

Surgical preparation, experimental protocol, and recorded variables. We used a subset of experiments carried out on chronically instrumented, conscious dogs to evaluate the effects of several experimental maneuvers on the cardiovascular variability series of R-R interval and SAP (21). The surgical procedure and the experimental protocol were described previously by Rimoldi et al. (21).

Briefly, all the dogs were chronically instrumented to measure electrocardiogram (ECG) and arterial pressure. Under anesthesia, the ECG electrodes were subcutaneously fixed to intercostal muscles (lead II). A catheter with strain-gauge transducers (Statham Instruments, Oxnard, CA) was inserted in the femoral artery and advanced to the abdominal aorta. In addition to ECG and arterial pressure, the respiratory movements were monitored by means of a thoracic belt connected to strain gauges. The respiratory signal was used to extract the breathing rate. In six dogs, a hydraulic occluder was positioned around the left circumflex coronary artery to occlude the artery when inflated with a volume of saline. In four dogs, TABD was performed in two steps. First, after both carotid artery bifurcations were identified, the sinus nerves were located and severed. Second, at the time of the thoracotomy, the adventitia surrounding the aortic arc and its branches was carefully dissected. Completeness of denervation was assessed by the loss of the usual heart rate response to pressure increases mechanically produced by occluding the distal thoracic aorta. Attention was paid to avoid visible damages to the vagi or to the sympathetic nerve branches.

Recordings were performed after a recovery period of 1-2 wk. All the dogs were acquainted with the laboratory and were trained to lie unrestrained on the recording table. Recordings were carried out: 1) under control conditions (n = 16), 2) 5-10 min after intravenous NT (32 µg · kg-1 · min-1) (n = 8), 3) during brief (2 min) CAO (n = 6), and 4) after TABD (n = 4). Experimental protocols were approved by the Committee on Animal Use and Care of the University of Milan.

At control conditions, mean R-R and SAP were 739 ± 128 ms and 126 ± 22 mmHg, respectively. After NT, a moderate hypotension (104 ± 13 mmHg) and a reflex tachycardia (539 ± 139 ms) were observed. During CAO, the decrease of R-R interval was even more marked (499 ± 44 ms), without marked changes in mean arterial pressure. After TABD, the R-R was 621 ± 179 ms and SAP strongly increased (167 ± 9 mmHg).

Beat-to-beat variability series extraction and baroreflex gain evaluation. ECG, arterial pressure, and respiratory signals were analog/digital converted at 300 Hz. The QRS peak was detected by using a threshold on the first derivative of ECG. Jitters in the location of the R peak were minimized by parabolic interpolation. The ith R-R measure was obtained as the temporal distance between two consecutive R peaks. The maximum of the arterial pressure inside the ith R-R interval was the ith SAP. The respiratory signal was sampled in correspondence with the first QRS defining the ith R-R interval.

Indexes of the baroreflex gain (alpha ) were derived directly from sequences of ~300 consecutive R-R intervals and SAP values by means of the proposed models (alpha X, alpha XAR, and alpha XXAR from X, XAR, and XXAR models, respectively). We also calculated alpha BS (10), alpha PS(LF) and alpha PS(HF) (19), and alpha CS(LF) and alpha CS(HF) (22).

Statistical analysis. Comparisons between control and other experimental conditions were performed by means of one-way analysis of variance (Tukey test). If the normality test was not passed, Kruskal-Wallis one-way analysis of variance on ranks was used (Dunn test).

The index alpha X was compared with alpha BS, alpha PS, and alpha CS in the same experimental condition by using one-way repeated-measures analysis of variance (Tukey test). If the hypothesis of normality was not fulfilled, Friedman one-way repeated-measures analysis of variance on ranks was used (Tukey test). This comparison is performed to evaluate the extent to which the estimate of the baroreflex gain changed when causality was imposed and variability sources different from SAP were disregarded. The same statistical analysis was used to compare alpha XXAR to alpha X and alpha XAR in the same experimental condition. This comparison was performed to evaluate the extent to which the estimate of the baroreflex gain varied when sources independent of SAP variations but capable of driving R-R interval changes were explicitly disentangled. A P < 0.05 was considered significant.


    RESULTS
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ABSTRACT
INTRODUCTION
CAUSAL PARAMETRIC MODELING...
TRADITIONAL APPROACHES TO...
METHODS
RESULTS
DISCUSSION
APPENDIX
REFERENCES

Estimating baroreflex gain from spontaneous beat-to-beat variability of R-R interval and SAP: an example. An example of beat-to-beat variability series of R-R interval and SAP under control conditions is depicted in Fig. 2, A and B. The power spectra (Fig. 2, C and D) point out that the R-R interval and SAP variabilities were dominated by a clear HF rhythm (at 0.23 Hz in this example) synchronous with respiration (not shown). The relevant K2 (Fig. 3) is close to 1 at HF and even at frequencies higher than HF. In contrast, K2 is <0.5 at frequencies lower than HF (from 0 to 0.1 in this example). Both the proposed causal parametric approach estimating alpha X, alpha XAR, and alpha XXAR and traditional methods producing alpha BS, alpha PS, and alpha CS were applied to this sequence of data.


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Fig. 2.   Beat-to-beat series of R-R interval (A) and SAP (B) in a conscious dog at control. The relevant AR power spectral densities exhibit a dominant high-frequency (HF) component at 0.23 Hz (C and D, respectively).



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Fig. 3.   Squared coherence function (K2) between the R-R and SAP series of Fig. 2. K2 is >0.5 at HF and <0.5 in the range from 0 to 0.1 Hz.

In Fig. 4 the response of the Hrr-sap block of the X, XAR, and XXAR models (Fig. 1, A, B, and C, respectively) to the unitary ramplike increase of sap is represented. Their least-squares fittings, the slope of which provided the estimate of the baroreflex gain (alpha X, alpha XAR, and alpha XXAR, respectively), were superposed. The X model provided the largest estimate of the baroreflex gain (alpha X = 48.9 ms/mmHg), whereas the smallest estimate was furnished by the XXAR model (alpha XXAR = 31.6 ms/mmHg). alpha XAR, based on the XAR model, was 41.2 ms/mmHg.


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Fig. 4.   Response of the Hrr-sap block to the ramplike increase of sap for the X (triangle ), XAR (open circle ), and XXAR () models calculated on the R-R and SAP series of Fig. 2. The slope of the linear fitting (solid lines) represents the estimate of the baroreflex gain (alpha X, alpha XAR, and alpha XXAR, respectively).

alpha BS is based on the detection of the baroreflex sequences present in the two series. In this set of data they are only 4%. All these sequences, when plotted in the plane (SAP, RR), appeared as straight segments (Fig. 5). These segments were covered from the lower left corner to the upper right corner for the positive sequences and in the opposite direction for the negative sequences. The index alpha BS = 54.2 ms/mmHg was obtained as the average slope of these segments.


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Fig. 5.   Straight segments representing in the plane (SAPi-1,RRi) the linear regression on the baroreflex sequences (both positive and negative) detected in the R-R and SAP series of Fig. 2. The mean slope is alpha BS.

alpha PS is based on power spectral analysis of R-R interval and SAP series and on the calculation of the power associated with spectral components. The HF components are represented in Fig. 6. The power associated with the HF components (Fig. 6, A and B) was used to evaluate an alpha PS(HF) = 39.2 ms/mmHg, whereas a consistent estimate of alpha PS(LF) was prevented by the absence of LF components of R-R interval variability. The reliability of the estimate of alpha PS(HF) was confirmed by the high degree of squared coherence (Fig. 3) at HF (KHF2 = 0.99).


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Fig. 6.   Spectral components at HF (filled area) relevant to the R-R (A) and SAP (B) power spectra calculated on the R-R and SAP series depicted in Fig. 2. The area (i.e., the power) of these components is used to estimate alpha PS(HF). No component is detectable in the low-frequency (LF) band in the R-R power spectrum (A).

alpha CS is based on the estimation of the SAP-R-R transfer function magnitude (Fig. 7). It was sampled at HF detected on the SAP series, thus producing alpha CS(HF) = 41.9 ms/mmHg. alpha CS(LF) could not be calculated consistently because KLF2 < 0.5 (Fig. 3). KHF2 > 0.5 confirmed the reliability of alpha CS(HF).


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Fig. 7.   Magnitude of the Hrr-sap transfer function between R-R and SAP series of Fig. 2. This function, sampled at HF, provides alpha CS(HF). It is not sampled in the LF band because the coherence function K2, depicted in Fig. 3, is <0.5 at LF.

Testing reliability of baroreflex gain estimates. The reliability of the baroreflex gain estimates based on the causal parametric approach depends on the ability of the model to produce white and noncorrelated residual signals. In the X model, wsap was always white, whereas wrr passed the whiteness test in 14 of 16 animals under control conditions, in 1 of 8 after NT, in 4 of 6 during CAO, and in 2 of 4 in TABD. These results pointed out that the structure of this model is too simple to describe the R-R interval dynamics. However, the two residual signals wrr and wsap in the X model were not correlated, even at zero lag, in any condition. The inability of the X model to describe the R-R interval dynamics is confirmed by the relatively low value of the goodness of fit rho rr (0.59 ± 0.16 at control, 0.59 ± 0.16 after NT, 0.45 ± 0.14 during CAO, and 0.57 ± 0.19 after TABD). When the structure of the model was rendered more complex (XAR and XXAR models), the tests on the whiteness of the residual signals and on their noncorrelation were fulfilled in all conditions. rho rr was increased accordingly in the XAR model (0.69 ± 0.13 at control, 0.71 ± 0.17 after NT, 0.75 ± 0.06 during CAO, and 0.76 ± 0.17 after TABD) and revealed the largest values in the XXAR model (0.78 ± 0.12 at control, 0.73 ± 0.16 after NT, 0.79 ± 0.06 during CAO and 0.81 ± 0.12 after TABD).

The reliability of alpha BS depends of the number of baroreflex sequences detected in the variability series. Under control conditions the mean percentage of baroreflex sequences (over 300 samples) was 5%. In 8 of 16 dogs the percentage was <3%, and in 4 animals no slope was present. An example of R-R interval and SAP beat-to-beat variability in which at least three contemporaneous increases or decreases of R-R interval and SAP were not present (no baroreflex sequence could be detected) is depicted in Fig. 8, A and B. The magnification of two periods of dominant HF rhythm (Fig. 8C) shows that, whereas three consecutive increases can be found in SAP series, R-R interval can increase or decrease only for two beats, thus producing the absence of baroreflex sequences. The percentage of baroreflex sequences was larger after NT (18%; only 1 dog exhibited <3%), during CAO, and after TABD (12% and 24%; no animal exhibited <3%).


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Fig. 8.   Example of R-R interval (A) and SAP (B) series in which no baroreflex sequence is found. Indeed, the magnification of 2 cycles of the dominant respiratory rhythm (C) present on the R-R (solid line) and SAP (dotted line) series demonstrates that 3 contemporaneous increases or decreases of R-R interval and SAP cannot be found.

The reliability of alpha PS(LF), alpha CS(LF), alpha PS(HF), and alpha CS(HF) was tested by evaluating the value of the squared coherence at LF and HF (KLF2 and KHF2). alpha PS(LF) and alpha CS(LF) could not be calculated in all animals because LF oscillations were not always found. Moreover, even when LF oscillations were observed, they exhibited a value of KLF2 > 0.5 only in a few cases (7 of 16 at control, 2 of 8 after NT, 5 of 6 during CAO, and 0 of 4 after TABD). In contrast, KHF2 was >0.5 in all animals in all the conditions (0.98 ± 0.03 at control, 0.95 ± 0.05 after NT, 0.91 ± 0.16 after CAO, and 0.98 ± 0.01 after TABD).

Causal modeling approach vs. traditional methods. The results are summarized in Table 1. At control, alpha BS, alpha PS(HF), and alpha CS(HF) were very high (>40 ms/mmHg). alpha PS(LF) and alpha CS(LF) were smaller and similar to alpha X and alpha XAR. alpha XXAR showed the smallest value, significantly smaller than alpha X and alpha XAR.

                              
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Table 1.   Summary of baroreflex gains estimated by traditional noninvasive methods [alpha BS, alpha PS(LF), alpha PS(HF), alpha CS(LF), and alpha CS(HF)] and by causal parametric models (alpha X, alpha XAR, and alpha XXAR) under different experimental conditions

All indexes diminished after NT, with alpha PS(LF), alpha CS(LF), alpha X, alpha XAR, and alpha XXAR comparable and smaller than alpha BS, alpha PS(HF), and alpha CS(HF). During CAO, the indexes alpha BS, alpha PS(HF), alpha CS(HF), and alpha X decreased significantly whereas alpha PS(LF), alpha CS(LF), and indexes based on more complex models (alpha XAR and alpha XXAR) exhibited a nonsignificant fall. It is worth noting that, during CAO, alpha XAR and alpha XXAR were comparable but significantly smaller than alpha PS(LF) and alpha CS(LF). After TABD, all the indexes showed a drastic reduction. However, only the indexes based on a causal parametric approach (alpha X, alpha XAR, and alpha XXAR) were close to zero. After TABD, alpha PS(LF) and alpha CS(LF) could not be calculated because of the lack of coherence in all animals.


    DISCUSSION
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All the methods considered here for estimating the baroreflex gain from spontaneous R-R interval and SAP variabilities are able to detect the decrease of the baroreflex sensitivity during baroreceptive unloading provoked by NT, during sympathetic activation induced by CAO, and after TABD, thus confirming the capability of these parameters to measure the baroreflex gain (Table 1). However, Table 1 points out that the values of the estimated baroreflex gains can be very different. These differences are the result of the different capabilities of the various methods to separate the baroreflex pathway from mechanisms capable of producing R-R interval and SAP variability independently of baroreflex circuit (Table 2). Three main mechanisms are responsible for R-R interval and SAP variabilities independent of baroreflex pathway: 1) Starling and windkessel effects producing SAP variations driven by R-R interval changes (i.e., the feedforward mechanisms), 2) neural modulations at HF capable of driving the R-R interval independently of SAP changes [e.g., neural influences projecting the activity of central respiratory oscillators (14) and neural reflexes involving low-pressure receptors activated by respiration-related changes in blood volume and central venous pressure (13, 28)], and 3) neural modulations affecting the sinus node at LF independently of SAP variations [e.g., neural influences projecting the activity of central slow oscillators (20) and cardiogenic reflexes initiated by ischemia]. Also, mechanical influences of respiration on sinus node produce R-R interval changes independent of SAP variations, but they are usually irrelevant [they become apparent in the denervated heart (9)].

                              
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Table 2.   Capability of baroreflex gain estimates to disentangle different regulatory mechanisms from baroreflex mechanism

Traditional methods for estimation of baroreflex gain. The indexes alpha PS and alpha CS (19, 22) are calculated without separating all these mechanisms from the baroreflex pathway (Table 2). Indeed, they are estimated without imposing any specific causal direction in the interactions between R-R interval and SAP variabilities (i.e., the feedforward mechanical path from R-R interval to SAP is merged with the feedback baroreflex pathway from SAP to R-R interval). In contrast, the index alpha BS (10) is actually calculated by separating the baroreflex sequences from the nonbaroreflex sequences, but no memory is allowed in feedback and feedforward relationships, thus preventing the full separation of feedback from feedforward influences (Table 2). As a consequence, the traditional indexes alpha BS, alpha PS, and alpha CS mix the gains of both paths and are closer to the baroreflex gain only if the R-R interval is mainly driven by SAP variations. This condition is more likely to be fulfilled at LF (2, 11). In contrast, R-R interval variability leads SAP oscillations at HF (2, 27), thus rendering alpha PS(HF) and alpha CS(HF) sensible to the mechanical pathway (i.e., the Starling and windkessel effects) and introducing a bias when these indexes are used to evaluate the baroreflex gain. According to this consideration, alpha PS(HF) and alpha CS(HF) can be different from alpha PS(LF) and alpha CS(LF), respectively, and can be significantly larger than 0 even after TABD (Table 1). Because the index alpha BS is not conceptually different from alpha PS and alpha CS, it could be more similar to alpha PS(LF) and alpha CS(LF) or to alpha PS(HF) and alpha CS(HF), depending on the predominant dynamics in the R-R interval and SAP variabilities. In dogs, as a result of a dominant HF dynamic in every experimental condition, alpha BS is similar to alpha PS(HF) and alpha CS(HF) (Table 1). These observations suggest the use of alpha PS(LF) and alpha CS(LF) instead of alpha BS, alpha PS(HF), and alpha CS(HF) in dogs and in other experimental preparations in which respiratory influences might directly drive the sinus node. Unfortunately, the presence of a small amount of R-R power in the LF band in dogs (21) makes it difficult to obtain a robust estimation of alpha PS(LF) and alpha CS(LF) (KLF2 is usually <0.5), thus rendering the estimate of baroreflex gain unreliable even in the LF band and necessitating new tools based on a causal modeling approach.

Role of causality in estimate of baroreflex gain. The proposed modeling approach fixes the temporal direction of the influences of SAP on R-R interval (i.e., causality), thus exploring the baroreflex pathway directly. Indeed, the R-R interval depends on SAP inside the same cardiac beat (fast effect) and on past SAP values (dynamic effect). The fast effect has been ascribed to the action of vagal circuits and the dynamic, slow effect to the sympathetic branch (12). This feature gives the model the possibility of separating the baroreflex pathway (the feedback path) from the mechanical relationship (mainly windkessel and Starling effects, the feedforward path) (Table 2). In other words, only that part of the R-R variability causally related to SAP changes is exploited to evaluate the baroreflex gain. As a result, alpha X, alpha XAR, and alpha XXAR are smaller than alpha BS, alpha PS(HF), and alpha CS(HF) in all experimental conditions, comparable to alpha PS(LF) and alpha CS(LF) under control conditions and after NT but significantly smaller during CAO and close to 0 after TABD.

Role of rhythmic influences independent of sap changes in estimate of baroreflex gain The simplest model (i.e., the X model) is able to evaluate the amount of R-R interval variability driven by SAP changes (i.e., the baroreflex-mediated R-R variability) but cannot model rhythmic inputs capable of driving R-R interval independently of SAP variations (Table 2). Therefore, alpha X is calculated without separating the baroreflex pathway from mechanisms [e.g., central slow oscillators (20), central respiratory oscillators (14), and cardiopulmonary reflexes (13, 28)] producing LF and HF oscillations on R-R interval not mediated by the baroreflex circuit (Table 2). In contrast, the XAR and XXAR models can disentangle the baroreflex pathway from mechanisms driving R-R interval independently of SAP (Table 2). The XXAR model can be considered a refinement of the XAR model (Table 2). Indeed, among the rhythmic sources driving R-R interval independently of SAP the XXAR model distinguishes those driven by respiration and, therefore, in the HF band, from those independent of respiration (i.e., in the LF band).

Under control conditions, alpha XXAR is significantly smaller than alpha X and alpha XAR, as a result of the effect of taking into account the respiration-related changes of R-R interval independent of SAP variations, which are particularly prominent in dogs (2, 4). During NT, alpha X, alpha XAR, and alpha XXAR are similar, as a result of a more important role of the baroreflex circuit in regulating R-R interval than that of central respiratory oscillators and low-pressure areas. During CAO, alpha X is significantly smaller than alpha XAR and alpha XXAR because of the technical inability of the X model to fit the data. The use of XAR and XXAR models allows us to solve the identification problem correctly and to find out that alpha XAR and alpha XXAR are similar. During CAO, the use of an XAR or XXAR model is necessary to take into account LF oscillations directly impinging on the sinus node as previously reported (4). In this experimental condition, XAR and XXAR models perform similarly because of the reduced importance of HF direct effects on the sinus node. It is worth noting that alpha PS(LF) and alpha CS(LF) remain significantly larger than alpha XAR and alpha XXAR as a result of the influence of LF fluctuations on R-R interval independent of SAP, thus pointing out that even in the LF band traditional indexes may be biased and making obvious the improvement of the causal model-based approach.

In conclusion, our data suggest that alpha XXAR provides a less biased value of baroreflex gain than any other indexes derived from sequence, power spectrum, and transfer function analyses or from simpler causal models. alpha XXAR is calculated by exploiting the R-R variability driven by SAP changes after disentangling different variability sources capable of producing changes in the R-R interval variability independent of the baroreflex circuit. If R-R variability was completely driven by SAP changes, traditional indexes would be equal to alpha XXAR. However, the former indexes may be larger than the latter because of the bias of direct effects of respiration on R-R variability, of slow fluctuations of R-R variability independent of the baroreflex circuit, and of the mechanical feedforward pathway. The estimation of alpha XXAR requires the additional recording of a respiratory signal but, in contrast to the sequence analysis, it uses all the information content of R-R interval series and, unlike spectral and transfer function analyses, it does not require the setting of specific frequency bands.


    APPENDIX
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In this appendix we summarize the methods used to estimate the coefficients of the X, XAR, and XXAR models, the power spectrum and the cross spectrum.

Identification and validation of X, XAR, and XXAR models. The coefficients of the X model (i.e., Eq. 1) and of the separate AR models describing the dynamics of sap and resp signals (i.e., Eqs. 2 and 6) are identified via a least-squares procedure (8, 15). The coefficients of the XAR model (i.e., Eqs. 3 and 4) and of the XXAR model (i.e., Eqs. 5 and 4) are identified using a generalized least-squares approach (8, 24). This iterative procedure is stopped when the current iteration does not produce a significant percent decrease in the variance of the residue wrr with respect to the previous one (the threshold is 0.001). The solution of both the traditional and generalized least-squares problems is performed by means of the Cholesky decomposition method (15).

The model adequately describes the dynamics of the signal if the residual signals (wrr and wsap for X and XAR models and wrr, wsap, and wresp for the XXAR model) are white (all the information is captured by the model parameters). The whiteness of the residual signals is verified by the Anderson test (15). This test checks that the normalized autocorrelation functions rho wrr(tau ), rho wsap(tau ), and rho wresp(tau ) (the autocorrelation functions divided by lambda wrr2, lambda wsap2, and lambda wresp2, respectively) are equal to 0 for tau not equal 0 and tau <= 40. If this is true for 95% of the values of tau , the test is fulfilled with 5% confidence, [e.g., with tau max = 40, rho (tau not equal  0 is allowed for <3 values of tau ]. The structure of the model is adequate to describe interactions among the signals if the residues are not correlated with each other (all relationships among the series are explained by the model structure). The same test used to check the whiteness of the residual signals is carried out to verify their noncorrelation; it checks that the normalized cross-correlation functions rho wrr-wsap(tau ) and rho wrr-wresp(tau ) (the cross-correlation functions divided by the product of the standard deviation lambda wrrlambda wsap and lambda wrrlambda wresp, respectively) are 0 for tau  <=  40 (even at tau  = 0). Obviously, in the case of X and XAR models, it is sufficient to test the whiteness of wrr and wsap and their noncorrelation. The choice of a high model order can help to fulfill these hypotheses. However, this solution should be avoided because the fitting is performed even on the noise superposed on the data. To favor small model orders, the model order is selected according to the minimum of the Akaike figure of merit for multivariate processes (1). The best model order is searched in the range from 6 to 16. After choosing the best model order, whiteness and noncorrelation on the residual signals are tested and the goodness of fit rho rr (i.e., Eq. 7) is calculated.

Power spectrum estimate. The power spectrum is calculated by using a parametric approach (18) instead of a nonparametric approach (3). The rr and sap series are described as AR processes considering the current value of the series as a linear combination of its p past values (e.g., see Eq. 2 for the AR model of sap). The coefficients of this linear combination are estimated via Levinson-Durbin recursion (15), and the number of the coefficients is chosen according to the Akaike criterion (1). The Anderson test is used to test whether the residue is white (15). After the power spectral densities of these two series are calculated, the power spectral decomposition procedure (29) is carried out to evaluate the contribution of each oscillation (described by a real pole or a pair of complex and conjugated poles) to the total power (i.e., the variance) of the process, thus allowing us to estimate the power in LF and HF bands.

Cross-spectrum estimate. The calculation of the cross spectrum between rr and sap series requires a bivariate approach instead of the monovariate approach required by spectral analysis. We choose a parametric approach based on a bivariate AR model (5) to estimate the autospectrum of sap series and the cross spectrum between sap and rr instead of a nonparametric method (11). The model order is fixed at 10, and the coefficients of the bivariate AR model are identified via least-squares methods (8, 15).


    FOOTNOTES

Address for reprint requests and other correspondence: A. Porta, Universitá degli Studi di Milano, Dipartimento di Scienze Precliniche, LITA di Vialba, Via G.B. Grassi 74 20157 Milano, Italy (E-mail: alberto.porta{at}unimi.it).

The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.

Received 13 December 1999; accepted in final form 20 May 2000.


    REFERENCES
TOP
ABSTRACT
INTRODUCTION
CAUSAL PARAMETRIC MODELING...
TRADITIONAL APPROACHES TO...
METHODS
RESULTS
DISCUSSION
APPENDIX
REFERENCES

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