1 Appendix S1 β Statistical properties of the abundance-weighted average 2 estimator for center of gravity 3 4 Several previous studies have used an βabundance-weighted averageβ estimator for the center of 5 gravity for a population in each year. This estimator averages the location of sample 6 observations si, where location is generally summarized using spatial coordinates, si = ( Lat(i), 7 Lon(i) )T, and where each location is weighted by the observed biomass at that location (where 8 other metrics, including counts of individuals or abundance have also sometimes been used): ππππ (π‘) π Μ (π‘) = β 9 π=1 ππ π π ππππ (π‘) βπ=1 ππ 10 where nobs(t) is the number of survey occasions in year t, ci is biomass (in kg.) for the i-th sample 11 in year t. Assuming that samples are proportional to local density, E(ππ ) β π(π , π‘), the expected 12 value of this estimator is a function of the sampling distribution function π«(π , π‘) and the species 13 density function d(s,t): 14 E(π Μ (π‘)) = β« π π«(π , π‘)π(π , π‘) ππ π(π‘) 15 where E(π Μ (π‘)) is the expected value for the abundance-weighted average estimator, and π(π‘) = 16 β« π«(π , π‘)π(π , π‘)ππ is an integration constant for total sample-weighted abundance. This equation 17 implies that E(π Μ (π‘)) will decrease if E(π π«(π , π‘)) decreases and vice-versa. Therefore, we 18 conclude a priori that the abundance-weighted estimator will result in biased estimates of trends 19 in the center-of-gravity whenever the sampling intensity function π«(π , π‘) itself has a spatial trend 20 over time. The expectation E(π Μ (π‘)) also includes population density d(s,t) only via its product 1 21 with sampling intensity π«(π , π‘), so we conclude that the two processes are perfectly confounded 22 by the estimator. 2 23 Appendix S2 β Calculating center of gravity, population boundaries, the 24 population kernel, and area occupied for the species distribution function 25 model 26 27 Our species distribution model involves estimating a species density function d(s,t) representing 28 population density at every location s and time t: 29 π(π , π‘) = Ξ¦(ππ (π π )T π·π + ππ (π π , π‘π )) × expβ‘(ππ (π π )T π·π + ππ (π π , π‘π )) 30 where this equation predicts density while accounting for spatiotemporal variation in encounter 31 probability p(s,t) and density when encountered r(s,t), but based upon reference values for 32 catchability variables (i.e., such that ππ,π = ππ,π = π; see Appendix S3 for symbol definitions). 33 The species distribution model therefore βfilters outβ the average effect of catchability covariates 34 upon observed catch rates when predicting densities and derived statistics. The species density 35 function can then be used to calculate metrics for monitoring shifts in species distribution, 36 including (1) center of gravity, (2) the area occupied by the core of the species distribution, and 37 (3) population boundaries. 38 1. Center of gravity 39 We are specifically interested in the center-of-gravity for the distribution of a given species: 40 π(πΏ(π‘)) = β« πΏ(π , π‘) π(π , π‘) ππ π(π‘) 41 where Ξ΄(s,t) is any measured variable that is useful for tracking changes in spatial distribution 42 over time, and π(π‘) = β« π(π , π‘)ππ is an integration constant representing total abundance in time 43 t. In the following, we track spatial changes in the center of gravity and therefore define 44 Ξ΄(s,t)=Latititude(s)¸or Ξ΄(s,t)=Longitude(s). 3 45 2. Area occupied 46 We also calculate the variance of the species density function (termed the βinertiaβ in Woillez et 47 al. (2009)): π(πΏπ (π‘), πΏπ (π‘)) = β«(πΏπ (π , π‘) β π(πΏπ (π‘))) (πΏπ (π , π‘) β π(πΏπ (π‘))) 48 π(π , π‘) ππ π(π‘) 49 The center-of-gravity and variance can then be used to estimate a kernel K(t) that provides a 50 second-order approximation to the spatial distribution of the species in time t: πΎ(π , π‘) = πππ(ππΎ , Ξ£πΎ ) β π(π , π‘) 51 52 where ππΎ (π‘) = (π(πΏππ‘(π‘)), π(πΏππ(π‘))) 53 54 T and Ξ£πΎ (π‘) = [ 55 π(πΏππ‘(π‘), πΏππ‘(π‘)) π(πΏππ‘(π‘), πΏππ(π‘)) ] π(πΏππ‘(π‘), πΏππ(π‘)) π(πΏππ(π‘), πΏππ(π‘)) 56 This kernel can then be summarized to visualize an ellipse that contains a fixed proportion p of 57 the area under the kernel approximation to population density d(t). This ellipse is indicated by 58 values: 59 |πΎ(π , π‘) β ππΎ (π‘)| = πΉ β1 (π, 2) 60 where |πΎ(π , π‘) β ππΎ (π‘)| is the effective distance of location s from the center of the population 61 ππΎ (π‘) in year t, and πΉ β1 (π, 2) is the chi-squared cumulative distribution function evaluated at 62 proportion p and with 2 degrees of freedom. 63 Hypothetically, a northward shift in population center-of-gravity might be caused by either 64 an expansion along the northern or a contraction along the southern boundary of the population. 65 Therefore, calculate an index of population area to distinguish between these two possibilities. 4 66 Specifically, we calculate an index of the area occupied by the population, where this index at in 67 year t is calculated: 68 ππ‘ = ππΉ β1 (π, 2)β|Ξ£πΎ (π‘)| 69 where |Ξ£πΎ (π‘)| is the determinant of the variance Ξ£πΎ (π‘) of the kernel approximation to the species 70 density function. 71 3. Population boundaries 72 Finally, we calculate a metric representing population boundaries along a pre-defined axis. To 73 do so, we calculate the cumulative distribution for population density along the axis (e.g., 74 northings), and use quantiles from this distribution (i.e., the 5th and 95th percentiles) as the 75 boundary along this axis. 76 The cumulative distribution is calculated by first extrapolating the density function to each of 77 15,979 grid cells within the domain of the triannual and annual surveys (each is 2x2 nautical 78 miles). Each cell is assumed to have density equal to the density of the nearest knot. We then 79 calculate the cumulative distribution: ππ‘ (πΏ) = 80 πππππ βππ=1 π(π π , π‘) πΌ(π π < πΏ) π(π‘) 81 where π(π π , π‘) is the extrapolated density for the jth cell (centered at location sj), ncells is the 82 number of cells, πΌ(π π < πΏ) is an indicator function that equals one if sj is less than πΏ and zero 83 πππππ otherwise, π(π‘) = βπ=1 π(π π , π‘) is an integration constant that ensures that π(πΏ, π‘) is one when 84 πΏ β β, and ππ‘ (πΏ) is the quantile function in year t, returning the proportion of abundance that is 85 located to one side or the other of πΏ. Once this cumulative distribution is calculated, we then 86 identify the lower and upper bounds such that 87 π 0.05 = ππ‘ (πΏπππ€ππ (π‘)) 5 88 89 90 and 0.95 = ππ‘ (πΏπ’ππππ (π‘)) but where other quantiles could also have been used. 91 6 92 Appendix S3 β Detailed description of methods for the spatiotemporal species 93 distribution function model 94 95 We seek to estimate a function d(s,t) representing density d at any given location s and time t. 96 This function is decomposed into the probability p(s,t) of encountering the species at a given 97 location, and the expected density r(s,t) of the species when encountered, where π(π , π‘) = 98 π(π , π‘)π(π , π‘). Each component is in turn modeled as a spatiotemporal process: 99 Ξ¦β1 (ππ ) = ππ (π π )T π·π + ππ (π π , π‘π ) + ππ,π πΈπ 100 log(ππ ) = ππ (π π )T π·π + ππ (π π , π‘π ) + ππ,π πΈπ 101 where encounter probability pi for sample i at location si and time ti is specified via a logit link 102 function Ξ¦β1, and encounter probabilities ri are specified via a logarithmic link function, x(s) is a 103 multivariate function representing measured covariates at location s and Ξ² is a vector of 104 coefficients estimated for variables x, Ξ΅(s,t) represents spatiotemporal variation in the species 105 distribution function, and zp,i and zr,i is a vector of variables affecting catch rates independent of 106 local densities (termed βcatchabilityβ variables) where Ξ³p and Ξ³r are vectors of coefficients 107 allowing catchability variables zp and zr to impact encounter probabilities and densities. 108 We constrain this function by invoking the First Law of Geography (Tobler 1970) wherein 109 nearby locations on average have greater similarity than geographically distant locations. We 110 therefore specify that spatial variation follows a stationary stochastic process that exhibits 111 geometric anisotropy, while temporal variation follows a random-walk process in time: 112 2 ππ (π‘)~πΊπ(ππ (π‘ β 1), ππ,π Cπ ) 113 where Cp is a correlation function governing the decrease in similarity in encounter probabilities 114 as a function of distance: 7 115 πΆπ (π , π + β) = πππ‘πππ(|πβ|; π π ) 116 and where H is a 2x2 matrix representing geometric anisotropy, h is a vector representing the 117 displacement of two locations s and s+h, and therefore |Hh| represents the effective distance 118 between these two locations (Thorson et al. 2015b), and where π π and π π are estimated to 119 represent the spatial scale of similarity in probability of encounter and positive density 120 components. Spatiotemporal variation ππ is defined similarly for positive catch rates. We chose 121 to use a random-walk temporal process, rather than an autoregressive process, to ensure that 122 locations and/or time intervals without sampling do not exhibit mean-reversion, which could 123 otherwise shrink center-of-gravity estimates for undersampled time periods towards the average 124 center-of-gravity for better sampled periods. However, we confirm that all results are 125 qualitatively similar when re-estimated via an autoregressive model where the magnitude of 126 autoregression is estimated as a fixed effect. 127 8 128 Appendix S4 β Details regarding a simulation experiment evaluating the likely 129 performance of AWA and SDF estimators 130 We conduct a simulation experiment to illustrate the magnitude of bias that arises from using 131 either the AWA or SDF estimators given the timing and location of samples that are available. 132 In this experiment, we simulate population density π(π , π‘) = π(π , π‘)π(π , π‘) in each of 15,979 grid 133 cells within the domain of the triannual and annual surveys (each is 2x2 nautical miles), where 134 each component is modeled as a spatiotemporal process: 135 π(π , π‘) = Ξ¦ (ππ (π , π‘) + ππ (π )) π(π (1); ππ (π‘), ππ ) 136 π(π , π‘) = expβ‘(ππ (π , π‘) + ππ (π ))π(π (1); ππ (π‘), ππ ) 137 where encounter probability p at location s and time t is specified as the logistic transformation 138 Ξ¦ of Ξ΅p(s,t) and Οp(s), representing spatiotemporal and purely spatial variation in encounter 139 probability (see Appendix S1 for more details regarding notation), and where the density given 140 encounters r is defined similarly except using an exponential transformation. Each component 141 also affected by a unimodal preference function based on the northings s(1) of location 142 s=(Northings,Eastings)T. We use a Gaussian probability density function π(π (1); ππ , ππ ) for 143 this preference function, where the northward center ππ (π‘) of this preference function varies 144 among years, thereby inducing shifts in the species center of gravity, and where the dispersion ππ 145 is fixed equal to one-quarter of the total range north to south of the population domain (402.5 146 km). 147 148 We explore model performance given four scenarios regarding changes in COG over time: 1. Constant β The preference function is constant for all years, ππ (π‘) = π, where π is the 149 average northings of the 15,979 grid cells. This scenario still has small interannual variation 150 in COG due to random variation in ππ (π , π‘) and ππ (π , π‘) among years. 9 151 2. Variable β The centroid of the preference function varies among years ππ (π‘)~π(π, ππ ), 152 where ππ is again one-quarter of the total range north to south of the population domain. 153 This induces high interannual variation in northward center of gravity. 154 3. Northward shift β The centroid of the preference function shifts progressively northward, 155 ππ (π‘) = β0.5ππ + (π‘ β 1)ππ /(ππ‘ β1), where nt is the number of years of data (37 years), 156 such that the centroid of the preference function moves northward 402.5 km over this period. 157 4. Southward shift β The centroid of the preference function shifts progressively southward, 158 ππ (π‘) = 0.5ππ β (π‘ β 1)ππ /(ππ‘ β1), in the mirror image of the Northward shift scenario. 159 160 Sampling data are then simulated as follows: ππ ~ππ πΏπ(log(π(π π , π‘π )) , ππ2 ) 161 where πΏπ(log(π) , π) is a lognormal distribution with log-mean a and log-standard deviation b, 162 and ππ indicates whether sample i encounters the species or not: 163 164 ππ ~π΅πππ(π(π π , π‘π )) where π΅πππ(π) is a Bernoulli distribution with probability a. 165 In this exercise, we simulate sampling to occur at the location and year of each sample in our 166 case study application, such that the sampling intensity function π«(π , π‘) is identical to that in our 167 case study. We also specify large residual variation in sampling data ππ = 1, moderate levels of 168 spatial variation, ππ,π = ππ,π = 0.5, and low levels of spatiotemporal variation, ππ,π = ππ,π = 169 0.2, where the range of spatial covariance is defined such that correlations are 10% at a distance 170 of 1000 km for encounter probabilities p, and 500 km for catch rates given encounters r. 171 10 172 Appendix S5 β Visualizing the spatial distribution of sampling for triennial 173 and annual surveys 174 175 Fig. S1 β Spatial distribution of sample locations for the triennial survey (red) and annual survey 176 (blue) in each year (the area without samples in the Southern California bight is a conservation 177 area that is excluded from sampling, and hence densities are not extrapolated into this area) 11 178 179 12 180 Appendix S6 β Changes in the northern and southern population boundary 181 for West Coast fishes 182 183 We here show estimates of the 5 and 95 percentiles of the northward cumulative distribution of 184 abundance for each of 18 West Coast species. The 50 percentile corresponds to the median of 185 the northward distribution, and this median shows similar trends to the center of gravity for most 186 species (Fig. 5 in main text). Several species show large shifts in the population boundary, 187 including Pacific hake, which has a north-skewed distribution in 1992 relative to other years. 188 Similarly, sharpchin and darkblotched rockfish show a northward movement of the southern 189 population edge. For darkblotched, this coincides with a northward shift in the population 190 center-of-gravity (Fig. 5 in main text), and corroborates a decrease in the area occupied by this 191 species (Fig. 7 in main text). 192 13 193 Fig S2 β The 5, 50, and 95 percentiles of the northward cumulative distribution function for each 194 West Coast species. 195 14
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