1. Introduction
Preservation of cultural heritage is an important activity of any civilized society. Pursuant to this, in recent years a wide array of non-destructive testing tools for evaluating the condition of various aspects of the built environment have been developed [
1,
2]. In particular, Lai et al. [
3] provide a detailed review of the history of ground-penetrating radar (GPR) use for civil engineering applications, that includes a comprehensive section on studies involving cultural heritage buildings.
In this work we discuss the interpretation of GPR data in an important historical context in which the ground-truth is mostly, although not completely, known. The interpretations described herein can serve as a guide to scientists who wish to better understand GPR data acquired at cultural heritage sites that are characterized by non-existent or poorly-known ground truth. There should be a sufficient range of interesting subsurface targets at the present study site to stimulate the interest of most GPR practitioners. The GPR data in this paper are minimally processed, on purpose, both to preserve the generality of the discussion and to provide reassurance that useful interpretations can be made without subjecting the data to an extensive technical workflow. An example of an advanced GPR workflow based on radar-signal amplitude analysis applied to a cultural heritage investigation may be found in [
4]. Additionally, radar signatures could be quantitatively modeled, for instance using wave-propagation simulation software such as gprMax [
5] or an equivalent. This is a worthy task that would provide additional valuable insights, but unfortunately it is outside the scope of the present study.
Ground penetrating radar (GPR) is often an appropriate geophysical tool for applications that favor high vertical resolution at the expense of deep penetration. GPR imaging is accomplished by detecting the subsurface electromagnetic impedance contrasts that govern reflections, diffractions and scattering of an electromagnetic wave generated by a transmitter, normally located at or near the ground surface. In the frequency range from 10 MHz to 2 GHz, wave propagation in resistive ( < 0.01 S/m) and non-magnetic () earth materials is mainly sensitive to spatial changes in dielectric permittivity ε in the subsurface. The radar signal becomes attenuated by any conductive material through which the wave propagates. With systematic movement of the transmitter and receiver antennas, the signals can be combined into an image of the subsurface objects and discontinuities from which the waves have reflected, diffracted, and/or scattered.
Selection of antenna frequency is important. For example, the well-known resolution vs. range tradeoff is discussed in Davis and Annan [
6]. The requirement of high resolution suggests that a high frequency antenna should be used, but high-frequency signals quickly attenuate and consequently have a smaller depth of penetration than lower-frequency signals. The GPR user must select a frequency that offers an acceptable tradeoff between resolution and depth of penetration. Some studies utilize a range of frequencies to obtain low-resolution information about deeper structures, along with higher-resolution information about shallower structures. For example, Utsi and Colls [
7] used 4 radar frequencies while prospecting different aspects of the subsurface environment beneath the Holy Trinity church floor at Stratford-upon-Avon in their investigation of the early 17th century Shakespeare burial site: 250 MHz (background soil structure); 400 MHz (deep graves to ~5 m depth); 1.5 GHz (shallow graves to ~1.5 m depth) and 4 GHz (possible grave goods and small metal artifacts associated with coffins). Furthermore, it should be noted that the GPR response of an elongated subsurface target depends on the orientation, or polarization, of transmitter and receiver antennas with respect to the long axis of the target [
8,
9]; an example of this effect is shown in the results section below.
There have been many previous studies using GPR to examine historical structures. Terenzi et al. [
10] used GPR to perform a structural integrity assessment of a heritage building located in an earthquake-prone region. Masini et al. [
11] and Johnston et al. [
12] used GPR at frequencies 1 GHz and higher to detect internal discontinuities and facilitate evaluations of the structural integrity of historic masonry walls, pillars and columns. In these studies, the GPR apparatus was directly applied to vertical surfaces to image the internal structure of above-ground infrastructure, rather than the more traditional subsurface inspection based on radar antennas placed on the ground, which is the configuration considered herein.
It is common for non-destructive techniques to be employed in order to characterize pre-existing buildings of historical significance that have subsequently been built upon [
13]. In this context, Udphuay et al. [
14] conducted a GPR survey at 500 MHz over the fine gravel floor of a Gothic abbey in southern France and mapped a number of subsurface features related to an underlying Romanesque building. Other GPR studies have identified hidden subsurface features that are essential structural components of visible above-ground items of cultural heritage. For instance, Miccinesi et al. [
15] used a stepped-frequency GPR to map beneath the floor of the Accademia gallery in Florence, Italy, and revealed the circular concrete foundation supporting Michaelangelo’s statue of David. Many other examples may be found in the literature.
In this paper, we demonstrate the interpretation of GPR images at a site in which a later building was built atop the basement of a pre-existing one, wherein both are now of historical significance. In many cultural heritage investigations at such locations, a certain type of historical subsurface structure is designated as a target of interest, such as a grave, a foundation, or a wall belonging to the pre-existing structure. However, the radar signature of a target of interest can be partially occluded by signatures of other nearby subsurface objects of lesser interest, which herein are referred to as “clutter”. It should of course be noted that clutter in one investigation may actually be a target of another investigation, and vice versa. While this paper focuses on general interpretation, in the companion paper [
16] we demonstrate the application of curvelet analysis [
17] as a means to separate the radar signatures of some prescribed Citadel targets from those of clutter, so that the former can be studied in relative isolation.
2. Materials and Methods
A GPR survey was conducted in June 2016 within the cellhouse of the main prison building on Alcatraz island in San Francisco County, California. This paper describes an investigation of GPR signals that were generated due to the presence of the basement of an earlier building, the Citadel, underlying the present-day cellhouse. Ground-truthing of the GPR signals was enabled over much of the surveyed area by direct observation as stair access to the Citadel is available, as well as by comparison to historical documents [
18] and publicly available lidar data acquired within the Citadel.
During the 19th century, Alcatraz island was fortified by the U.S. Army to guard the San Francisco Bay area against potential attackers arriving by sea. Construction of the defensive barracks referred to as “The Citadel” begun in 1853 and completed by 1859 (
Figure 1a). During the subsequent building of the main prison (1908–1912;
Figure 1b) the upper two stories of the Citadel were removed, with only its basement and the surrounding dry moat included within the architectural plan of the overlying cellhouse. The surviving Citadel basement and dry moat beneath the cellhouse is probed by GPR in this study. Thompson [
19] provides a detailed history of Alcatraz island. A previous GPR survey of Alcatraz civil war-era fortifications located outside the main prison building was reported by de Smet et al. [
20].
GPR data were collected on the floor of the cellhouse in nine areas known as Sunrise Alley, Michigan Avenue, Broadway, Park Avenue, Sunset Strip, Library, South ABC-blocks, Barbershop and Times Square (
Figure 2). The surveyed areas are shaded and occupy easily accessible areas between and at the end of rows of the prison cells. It was not feasible to acquire GPR data within the confined spaces of the individual cells. The dataset was acquired during overnight hours while there were no visitors at this popular tourist destination (
Figure 3). Barbershop and Times Square radar coverage will not be emphasized in this paper since those areas lie wholly outside the footprint of the Citadel, as indicated in
Figure 2. South ABC-blocks is not located within the original Citadel footprint, per se, but is included herein since it overlies the “cistern additions area” (described below) that was built prior to 1882.
The structural elements of the Citadel have been altered several times by renovation and reinforcement works, including 1909 modifications for the new prison and extensive seismic upgrades in 2003 and 2014. These alterations are described in [
21]. There is no attempt made in this paper to discriminate, based on the observed radar signatures alone, between an original structure and a later renovation or modification. Such a discrimination would have to involve detailed knowledge of the materials and construction techniques used, perhaps an estimate of the expected level of environmental degradation, and definitely supported by some element of ground truth discovery. In general, however, unexpected or unusual radar signatures could provide cultural heritage investigators with important clues that an original structure has been modified.
The equipment used for the acquisition of GPR data was the Sensors and Software
© PulseEkko Pro Receiver (Model 1600) with a 100-V transmitter and 500 MHz electric-dipole antennas. Acquisition parameters included a stack number of 8 and a 100 ns time window for each trace. The processing steps included only a dewow filter to remove non-informative low-frequency signal energy, SEC gain to compensate for the signal energy loss caused by geometric spreading of the spherical wavefront, and in some cases a background subtraction to exclude the direct ground response and transmitter-receiver coupling. These standard procedures are explained in [
23]. Lines of GPR data were acquired by traversing the length of conveniently divided sections of the cellhouse floor. Once the end of a line was reached the next line was offset by either 0.25 m or 0.50 m, depending on the coverage area, and the acquisition proceeded in alternating directions until the full area was covered. Where an obstacle, such as a pillar preventing data acquisition, was encountered, a portion of the line was skipped, with the location of the obstacle noted.
The raw GPR data were not correctly oriented for immediate analysis, as alternating lines were acquired in opposing directions. In addition, some lines were split into multiple parts by obstacles. Some lines in the same coverage area were of different lengths due to the irregular dimensions of our partition of the accessible cell house floor, or slight irregularities in the along-profile trace sampling interval. The GPR data were first rectified so that all lines within a given coverage area were oriented in the same direction and, where appropriate, “rubber-band” interpolated [
23] to become equal in length. In the case of obstacles, the display was modified with the missing segment(s) masked out.
In this study, the GPR data were compared to publicly available terrestrial laser scanning (lidar) data from inside the Alcatraz citadel. The lidar data, acquired in 2016 by Paul Davidson of the National Park Service, proved indispensable in identifying the causative structures generating signals in the GPR data. The identification is accomplished by comparing the lidar scans with both GPR sections and time/depth slices created in PulseEkko software, provided by the radar equipment manufacturer. Further interpretational aid was provided by comparisons of the GPR depth-slices (C-scans) and vertical cross-sections (B-scans) to a number of publicly available historical, architectural and engineering documents. Note that the C-scans are presented as either time-slices or depth-slices, and the vertical axes of the B-scans are marked as either depth or two-way travel time. In all cases, a radar velocity of 0.1 m/ns was used to convert time to depth.
3. Results
A 2016 lidar rendering of the Citadel floor is shown in
Figure 4. Although the Citadel and overlying cellhouse are oriented at an oblique angle to the cardinal directions, herein for convenience we designate “north” as the direction pointing to the left in
Figure 4. Thus, with reference to the cellhouse floor plan (
Figure 2), north also points to the left such that, naturally, Sunrise Alley is on the eastern side and Sunset Strip is on the western side. Additionally shown in
Figure 4 are the locations of the radar profiles (B-scans) mentioned in the text, labeled by the appropriate figure number in which they appear.
A rendering of the Citadel structure along with the cistern additions areas is shown in
Figure 5. Marked on the figure are some of the principal targets identified in radargrams as well as the South ABC-blocks radar coverage area. In the next sections of the paper, GPR interpretations from the various Citadel-related radar coverage areas are provided.
Depth slices, along with an interpreted B-scan along Sunrise Alley, are shown in
Figure 6a. The radar signatures of two slender ceiling beams extending across the width of the surveyed area are easily seen in the depth slices (
Figure 6a, top), with a third one truncated by the stairs to the dungeon. In the B-scan (
Figure 6a, bottom), the three beams disrupt the flat-lying reflector at 1.5 m depth, caused by the ceiling of the underlying SE bastion of the Citadel. The bastion was designed to defend against intruders coming down the adjacent stairs into the dungeon. The large, complex hyperbolic reflectors disrupting the floor reflector at 2.7 m (apparent) depth are likely caused by two unusually shaped arched columns (
Figure 6b) located inside the bastion. The height of the room, from floor to ceiling, is apparently only 1.2 m, but it must be remembered that the floor reflector will be “pulled up” relative to the ceiling reflector since the electromagnetic wave velocity in air (~0.3 m/ns) is higher than the value (0.1 m/ns) used to achieve the B-scan time-to-depth conversion. The velocity pull-up phenomenon is described in [
24].
At the far right of the Sunrise Alley B-scan (
Figure 6a, bottom), the small hyperbolic event may be due to a reflection from a structure associated with the late-19th-century “cistern additions” (see
Figure 5). This area, now inaccessible and hence without ground truth, was used to store water since the island has no natural water resources. At the left of the depth slices is the location of a series of “dungeon cells” (later these became storage rooms) with vaulted ceilings. The radar profile at
y = 0.0 m in
Figure 6a, bottom, does not pass directly over the vaulted cells, but rather over the corridor in front of them, which explains why they do not exhibit a radar signature.
However, in another Sunrise Alley partial B-scan at
y = 3.5 m (
Figure 6c, bottom), hyperbolic radar signatures of two of the vaulted ceilings are indeed apparent, they are marked as A,B. The signatures are relatively faint since the electromagnetic wave has to pass through a thick section of masonry between the cellhouse floor to reach the top of the vaulted structure. The apices of the hyperbolae are located at the correct depth of 1.0 m, and are spaced by the requisite 2.5 m. The vaulted structures themselves may be seen in the lidar data (
Figure 6c, top). Possible signatures of the other two vaulted ceilings are hinted at in the B-scan, faint hyperbola appear immediately beneath the shallow reflector at C, below which electromagnetic signal does not penetrate effectively. The cause of reflector C is not known, but it could be associated with a metal pipe, or alternatively, construction material within or just below the cellhouse floor, such as steel plate, acting as an excellent radar reflector. Reverberations caused by the floor material of the cellhouse in this location could explain why the tops of the vaulted ceilings appear to be pulled up beneath reflector C. The prominent horizontal event D in the B-scan is unexpectedly strong, but in good alignment with the bottom of the ceiling beam, as shown in the lidar image.
Depth slices, along with an interpreted B-scan along Michigan Ave, are shown in
Figure 7a. Radar signatures of at least four steel beams in the ceiling of the prison “shower room” may be seen at the left side of the B-scan and on both depth slices. The shower room, open to visitors, occupies the same level as the Citadel basement (for the floorplan) [
25]. The two areas, however, are not connected but rather separated by a ~6-m wide zone bereft of radar reflectors which is herein interpreted as the undisturbed bedrock, specifically called “Alcatraz terrane”. Geologically, the bedrock is an early Cretaceous graywacke sandstone associated with the subduction of the ancient Farallon plate beneath North America [
26].
At the right of the Michigan Ave. B-scan resides the cistern additions area wherein several small, shallow hyperbolic reflectors are found; these could mark structures that partition the water storage area, or they may be caused by objects such as pipes or taps related to the water supply. Their signature is also seen in the shallowest (0.10–0.15 m) depth slice. The Citadel itself lies at the center of the Michigan Ave. radar profiles. The “dry moat” that surrounds the Citadel outer walls, as well as the “middle aisle” of the structure itself, are easily discerned in both the depth slices and the B-scan. The middle aisle is labeled “Hall. Officers Quarters” and the rooms in between are labeled “Kitchens” or “Store-rooms” on the 1859 drawing [
27].
The distinctive fine-scale lineations, evident in the depth slices, are caused by wood planks that have been placed in the ceiling above the middle aisle and the dry moat of the citadel. A section of the ceiling exposing the wood planks is shown in the lidar data of
Figure 7b, left. The radar signature of the iron strapping holding the wooden planks in place is also evident; in the GPR depth-slice (
Figure 7b, right), the strapping appears to span across the 1859 kitchen, between the aisle and the moat. Note that the area of fine-scale lineations on the depth slices extends to the region
~45–47 m; these “extra wood planks” occur because the dry moat beneath this radar profile projects around the SE bastion (see
Figure 4). GPR non-destructive imaging of wood structures is becoming important in cultural heritage investigations [
28] as well as forestry and agriculture applications [
29,
30].
Depth slices, along with an interpreted B-scan along Broadway, are shown in
Figure 8. The GPR response is very similar to that of Michigan Ave. The similarity is expected as the lidar data, historical documents, architectural drawings, and also direct observations inside the Citadel show that the radar profiles pass over the same structures, namely the shower room, the undisturbed Alcatraz terrane, the dry moat, the Citadel structure and the cistern additions area. The knowledge that similar ground-truth generates similar radar signatures is important to keep in mind when working at cultural heritage sites where only partial ground-truth is available. It means that radar-signature interpretations from ground-truthed areas can be extrapolated into non-ground-truthed areas that exhibit analogous radar signatures.
The depth slices from Park Ave. are similar to those of Broadway and Michigan Ave. and hence are not shown here. However, note that the representative Park Ave. B-scan (
Figure 9, bottom) has a narrower region of undisturbed Alcatraz terrane rock and a wider (double) zone of moat than the profiles previously discussed. This is because the dry moat projects outward around the NW bastion of the Citadel (see
Figure 4). The B-scan also provides important information about the determination of the heights of underground structures. A N-S architectural cross-section [
25], spanning the shower room to the Citadel, is shown in
Figure 9, top. From this cross-section, it is evident that the ceilings of the shower room and the Citadel are at the same elevation. However, the height of the shower room is ~3.0 m while that of the Citadel is smaller, at ~2.4 m. Thus, the floor of the Citadel is at a higher elevation than the floor of the shower room.
The floors of the shower room and the Citadel show up as prominent flat-lying reflectors in the Park Ave. B-scan (
Figure 9, bottom). The Citadel floor reflector appears at a two-way travel time of 27 ns, while the shower-room floor reflector appears later at 34 ns. Given the known heights of the two rooms from the architectural cross-section, these travel-time values are consistent with a 1.0-m thick ceiling of radar velocity 0.1 m/ns in the shower room, and a 0.8 m thick ceiling of velocity 0.1 m/ns in the Citadel; values that seem reasonable from the perspective of masonry and concrete construction materials and techniques [
31]. There is of course a tradeoff between ceiling thickness and material velocity that could yield the same two-way travel time of a floor reflector for different combinations of these parameters. Specifically, the elementary principle applies to the travel time
being equal to the quotient of material thickness
and material velocity
, such that
.
Depth slices, along with an interpreted B-scan along Sunset Strip, are shown in
Figure 10a. At the left side of the depth slices, ceiling beams associated with the “clothing issue room” at the west end of the shower room are evident. A flat-lying reflector, corresponding to the floor of this room, is also seen at ~32 ns of two-way travel time in the B-scan. The reflector marked A in the B-scan may be caused by a laundry table in the clothing issue room. The section of undisturbed Alcatraz terrane rock between the clothing issue room and the Citadel appears, as usual, without significant internal radar reflections. In strong contrast is the dramatic radar signature of the metal trap doors, and underlying air space, at the top of the stairs leading down to the Citadel. The metal doors, shown in
Figure 10b, left, were closed shut at the time of the GPR survey. The radar profile that generated the B-scan passed over the edge of the closed trap doors, along the red line shown in the figure. Strong reflections, diffractions and reverberations are evident in the B-scan. The flat-laying series of reflectors at two-way travel time ~20–27 ns in
Figure 10b, right, are likely caused by the underside of the trap doors. Note that the radar signature beneath these reflectors tends to be less well-resolved but is otherwise a geometric copy of the radar signature above them, indicating reverberations of the electromagnetic signal between the upper and lower surfaces of the metal comprising the trap door. A smooth metal surface is an excellent reflector of radar signals [
32]. Finally at Sunset Strip, evident at the right-side of the depth slices and the B-scan (
Figure 10a), are ceiling beams spanning the dry moat of the Citadel.
Depth slices, along with two interpreted B-scans acquired in the Library, are shown in
Figure 11a. The library overlies the SW corner of the Citadel comprising the dry moat, several dungeon cells with vaulted ceilings, and three smaller rooms marked “Men’s Privy” on the 1859 drawing [
27] (see also
Figure 5). The fine-scale lineations, parallel to the
y-axis, seen most clearly in the two shallowest depth slices (
Figure 11a, upper left), correspond to wood planks in the ceiling of the dry moat. The planks show up as the near-surface zig-zag reflectors in the B-scans at
Figure 11a. The B-scan at the left also shows the hyperbolic signatures of the vaulted ceilings of the dungeon cells (compare with the same features in the Sunrise Alley B-scan of
Figure 6b, bottom), although these signatures are not apparent in the depth slices.
The other B-scan in
Figure 11a (bottom right) includes a very strong reflector labeled A at ~25 ns two-way travel time. This reflector lies at or near the base of the dry moat, but it is much stronger than a typical reflector from the floor of the moat. It is unclear why there is such a strong reflector in this part of the moat, although it might be related to the historic sewage disposal system. This supposition requires further investigation, but it is known from historical documents that the sewage from the cellhouse was directed via a pipe into a tunnel at the base of the easternmost privy, which is located at the right-side of the B-scan. From there, the sewage was discharged into San Francisco bay. Note that the privy itself is not imaged in the B-scan, perhaps because of its thick masonry ceiling. The privies, like the vaulted cells, lie outside the main Citadel structure (see
Figure 5) and extra ceiling reinforcement was probably installed for defensive purposes.
Another B-scan from the Library is shown in
Figure 11b, bottom. It contains a strong near-surface sequence of reflectors. These reflectors are aligned with a pair of iron pipes that are evident in lidar scans of the ceilings of interior rooms of the Citadel (the pipes are shown in
Figure 11b, top). The larger of the pipes appears to be connected to the pipe that is presently found on the easternmost privy floor. The pipe can be seen in
Figure 4, cutting diagonally across the moat.
Depth slices, along with two interpreted B-scans acquired at South ABC-blocks, are shown in
Figure 12. Most of the radar coverage passes over the cistern additions area, as indicated in
Figure 5, except for several meters on the western side. The original cisterns were built to provide water for the island staff and prisoners, but these proved inadequate and an additional area to house additional cisterns had been established by the late 19th century [
21]. There is no ground-truth available beneath the south-ABC blocks radar coverage area.
The depth slices in
Figure 12, top, show a prominent linear N-S anomaly stretching across the width of the coverage area at location
y~20 m, along with a fainter one at
y~8 m. The signature of their causative structures is evident in the B-scans along the lines
x = 7.0 m and
x = 2.0 m at
Figure 12, bottom. Specifically, the B-scans show two vertical linear sequences of strong hyperbolic reflectors, extending the entire depth range. These signatures are characteristic of multiple reverberations, or “ringing”, from a narrow metal reflector. Such a signal could be caused, for example, by a metal cover placed over a roof entry point into one of the cistern-area chambers; this manner of entry into the chambers is suggested on the 1859 drawing [
27]. The signals appear too strong to be caused by a less reflective cover material such as wood, brick or masonry, or an open hole. The linear anomalies in the depth slices are elongated and straight; these could be caused by some type of structure that provided access to entry points in the roofs of the chambers. The entry points themselves would correspond to the “bright spots” on the depth slices.
The rendering in
Figure 5 also suggests that 5 or 6 cistern chambers should be evident in the South ABC-blocks coverage area. A closer examination of the B-scans
Figure 12, bottom, shows that other near-surface hyperbolic reflectors are indeed present, although none of them generate a vertical sequence of strong reflectors. There also appears to be a number of broad-scale (width, Δ
x~3–4 m) faint hyperbolic reflectors at depth ~1 m, especially in the B-scan at the lower right. Whether or not these faint reflectors are associated with actual cistern chamber roofs requires further investigation.
Depth slices from Times Square along the north margin of the cellhouse are shown in
Figure 13 (left two panels). Although this area is outside the Citadel footprint, the radar signatures are examined here since they illustrate an important aspect of interpretation that should be of interest to cultural heritage investigators. The Times Square data were acquired along E-W lines running parallel to one of the long ceiling beams in the underlying shower room. The radar signature of the ceiling beam is highlighted by the white rectangles in the left two panels. Note that there are also a number of linear features running N-S beneath Times Square. However, here the focus is on the E-W ceiling beam extending almost the full length of the survey area. In
Figure 13 (right panel), the intersecting portions of depth slices from several areas with N-S oriented acquisition lines (Michigan Ave., Broadway and Park Ave.) are shown. The direction of data acquisition in these surveyed areas is perpendicular to the long ceiling beam in the shower room. Notice that the radar signatures of the ceiling beam in these areas are much more distinct than the signature of the same structure from the Times Square acquisition. In general, the radar signature of an elongated target is much more prominent in the case where the acquisition line is oriented perpendicular to the long axis of the target, as opposed to acquisition oriented parallel to the target. This is a well-known GPR polarization phenomenon. The physics underlying GPR polarization phenomena is described in detail by Roberts and Daniels [
7]. Note that the ceiling-beam signatures shown in
Figure 13 (right panel) are not precisely aligned with each other. Small misalignments such as these are expected, since the GPR antennas and their housings are of finite size and separation, and moreover the acquisition unit is sometimes difficult to precisely maneuver when it is close to walls and other obstructions.
4. Discussion
A composite GPR depth-slice from all 9 surveyed areas is shown in
Figure 14. This figure provides a synoptic view of the radar signatures of the subsurface structure beneath the cellhouse, including the Citadel and its dry moat, the Alcatraz terrane, the cistern additions area, and the shower room with the adjoining clothing issue room. Clearly, the depth slice is extremely rich in detail and, in this paper, only a first-order interpretation has been made of some of the primarily observed radargram features. The reader will probably observe a number of unexplained features in
Figure 14, and different features will become apparent if a different depth range is selected to display. Moreover, a thorough analysis of ground truth and historical documents, not to mention the performance of additional types of non-destructive testing, would yield additional insights beyond those offered in the present paper.
The complexity of GPR radargrams makes accurate and reliable interpretation a difficult task, especially where there is a lack of knowledge regarding characteristics of the structure under investigation such as the construction techniques used, the architectural plans of the original building and those of later modifications or refurbishments, the building materials involved and their current state of environmental degradation [
1]. Advanced GPR processing techniques are definitely useful to practitioners in assisting the interpretation of the causative structures that provoke interesting radar signatures at a given cultural heritage site. This paper has presented only minimally processed time/depth slices and B-scans, and from these a great deal has been learned, but additional processing steps such as spatial-wavenumber filters, velocity analysis, migration and attribute analysis [
23], if done carefully, in some cases could help to further resolve actual target structure and reduce contamination from clutter signatures and the effects due to wave propagation. While it is not the intent of the study to demonstrate the benefit of any or all of these useful techniques, an example of advanced processing is shown in the
Appendix A, and in the companion paper further analysis of representative B-scans from the Alcatraz citadel is performed using curvelet methods.
The ground truth which underlies the radargram interpretations presented herein comprises mainly the 2016 lidar dataset, in addition to a few key historical documents and architectural drawings. In many cultural heritage investigations, historical information is relied upon as the primary aid to GPR radargram interpretation within subsurface areas that are not directly accessible. This approach was taken for analysis of the GPR data from the cisterns additions area, for example, where lidar is not available. In general, “ground truth” comes in many forms—lidar scans, photographs, stories, drawings, oral histories, accidental exhumations, planned excavations, etc. There is a copious reservoir of such information about Alcatraz that we have not tapped into in this study, but which surely contributes to the rich knowledge we have of the Citadel and its significance in the context of history of the American west. The purpose of this study is not to add further insight to the fascinating history of the fortress lying beneath the main prison building at Alcatraz but rather, as mentioned, to serve as a useful reference for ground-penetrating radar interpretation that can be used at other multi-level cultural heritage sites.
Early on in the development of GPR for subsurface investigations, in the field of hydrogeology, Beres and Haeni [
33] presented a classification of radar signatures that turned out to be extremely useful for stratigraphic interpretation. Distinctive patterns and textures characterizing an individual radargram, or a portion thereof, were associated with distinctive sedimentological structures such as thin beds, cross-bedded strata, hummocky surfaces, gravel deposits, boulder fields, etc. These patterns and textures later became known as “radar facies” [
34,
35] in analogy with the “seismic facies” long known from seismic interpretation particularly within the oil and gas exploration industry. Similarly, in this paper we have seen distinct signatures from well-defined targets; the signatures from the wood planks and the vaulted ceilings being two examples of putative “cultural heritage” radar facies (see
Figure 15). A classification or compilation of common cultural heritage features, such as these, into a comprehensive facies classification scheme would be a logical extension of the work presented in this paper aiming at the development of a practical guide to field investigations.