DOI:10.2214/AJR.05.0804
AJR 2006; 187:W333-W340
© American Roentgen Ray Society
Intraoperative Triple Antenna Hepatic Microwave Ablation
Caroline J. Simon1,
Damian E. Dupuy1,
David A. Iannitti2,
David S. K. Lu3,
Nam C. Yu3,
Bassam I. Aswad4,
Ronald W. Busuttil5 and
Charles Lassman6
1 Department of Diagnostic Imaging, Brown Medical School, Rhode Island Hospital,
593 Eddy St., Providence, RI 02903.
2 Department of Surgery, Brown Medical School, Rhode Island Hospital,
Providence, RI.
3 Department of Diagnostic Imaging, David Geffen School of Medicine at UCLA, Los
Angeles, CA.
4 Department of Pathology, Brown Medical School, Rhode Island Hospital,
Providence, RI.
5 Department of Surgery, David Geffen School of Medicine at UCLA, Los Angeles,
CA.
6 Department of Pathology, David Geffen School of Medicine at UCLA, Los Angeles,
CA.
Received May 11, 2005;
accepted after revision August 12, 2005.
This research was sponsored in part with a grant from Vivant Medical Inc.,
Mountain View, CA.
Address correspondence to D. E. Dupuy
(ddupuy{at}lifespan.org).
WEB
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Abstract
OBJECTIVE. Microwave ablation is emerging as a new treatment option
for patients with unresectable hepatic malignancies. This two-center study
shows the results of a phase 1 clinical trial of patients with known hepatic
masses who underwent synchronous triple antenna microwave ablation before
elective hepatic resection.
SUBJECTS AND METHODS. Intraoperative microwave ablation was
performed before hepatic resection. Hepatic lesions were targeted using
real-time intraoperative sonography with three microwave antennas positioned
in a triangular configuration. Microwave ablation was performed at 45 W for 10
minutes. Hepatic resection was then completed in the standard fashion. Gross
specimens were sectioned and measured to determine tumor and ablation sizes.
Representative areas were stained with H and E stain and vital histochemical
nicotinamide adenine dinucleotide (NADH) stain.
RESULTS. Ten patients with a mean age of 64 years (range, 48-79
years) were treated. Tumor histology included colorectal carcinoma metastases
and hepatocellular carcinoma. The mean maximal tumor diameter was 4.4 cm
(range, 2.0-5.7 cm). The mean maximal ablation diameter was 5.5 cm (range,
5.0-6.5 cm), while the average ablation zone volume was 50.8 cm3
(range, 30.3-65.5 cm3). Gross and microscopic examinations of areas
after microwave ablation showed clear coagulation necrosis, even surrounding
large hepatic vessels (> 3 mm in diameter). A marked thermallike effect was
observed with maximal intensity closest to the antenna sites. NADH staining
confirmed the uniform absence of viable tumor in the ablation zone.
CONCLUSION. This study shows the feasibility of using multiple
microwave antennas simultaneously in the treatment of liver tumors
intraoperatively. Additional percutaneous studies are currently under way to
investigate the safety and efficacy in treating nonsurgical candidates.
Keywords: liver metastases microwave ablation radiofrequency ablation radiologic-pathologic correlation
Introduction
Hepatic tumors, whether primary or secondary in nature, remain a difficult
management challenge for all clinicians. In 2005, it was predicted that there
would be more than 667,000 new cases of liver cancer throughout the world with
more than 17,000 of the cases occurring in the United States alone
[1]. The most common type of
primary liver cancer is hepatocellular carcinoma (HCC), making it one of the
most prevalent and fatal of all malignancies. Although its incidence in the
United States continues to rise, only up to a third of patients are suitable
candidates for hepatic resection at the time of presentation
[2]. In addition, of the
estimated 145,000 new cases of colorectal cancer in the United States in 2005,
25% of these patients will have underlying metastatic disease at the time of
clinical presentation, with an additional 20-25% developing metastases within
a 5-year interval [1]. Again,
only a minority (10-20%) of these patients with hepatic colorectal carcinoma
(CRC) metastases will be candidates for liver resection
[1].
Given the unresectability of most liver neoplasms at the time of diagnosis,
local thermoablative techniques have been widely researched and integrated
into the treatment and management of these patients.
In 2003, a new microwave ablation system was engineered in the United
States [3]. Advances
incorporated into this system included the specific tuning of microwave
antennas to the dielectric properties of liver tumors, thus reducing feedback
while increasing the amount of energy deposited in the surrounding tissues. In
vivo experimentation with porcine liver using triple antenna ablation produced
synergistically larger ablation lesions
[4] than those produced by
single antenna ablation, thus hinting at the more convenient and effective
treatment of large tumors using microwave ablation. A novel microwave loop
antenna has also been studied in the single and double (parallel and
orthogonal) configurations with reports of precise and effective targeting in
in vivo porcine tissue [5].
In this article, we report our ablate and resect observations with
pathologic correlation using this new microwave ablation device with a triple
straight antenna design to treat liver tumors. Specifically, our primary aim
was to evaluate the size and microwave ablation characteristics in both
hepatic neoplasms and the adjacent normal liver parenchyma.
Subjects and Methods
Patient Population
This was a joint study performed at two tertiary cancer treatment centers
in the United States. The prospective study was approved by the respective
institutional review boards. From May 2003 to January 2004, 20 patients with
liver masses who were to be scheduled for curative liver resection were
identified and subsequently enrolled in this ablate and resect study. Ten
patients underwent microwave ablation with the triple antenna configuration
and were included in this study. Relevant patient exclusion criteria included
patients who had lesions ablated using single or double microwave antenna
configurations and a patient diagnosed with focal nodular hyperplasia.
Additional patient and tumor characteristics are summarized in
Table 1.
Informed consent was obtained from all the patients. The patient population
consisted of an equal number of men and women with a mean age of 64 years
(range, 48-79 years). All patients had undergone either multiphase CT or
gadolinium-enhanced MRI to delineate the target tumor and to assist with
surgical planning. The initial diagnosis of liver malignancy was based on
preoperative tissue biopsy, classical imaging characteristics of tumor
hypervascularity, or both and was correlated with the relevant clinical and
surgical history of the patient.
Microwave Ablation System
The microwave ablation system used was the VivaWave Microwave Coagulation
System (Vivant Medical). Three microwave generators were used, each capable of
producing up to 60 W of power at a frequency of 915 MHz. Each generator was
connected to a microwave antenna using a coaxial cable. The three single
microwave antennas were then arranged in a three-probe triangular clusterlike
configuration, spaced (using a rigid spacer supplied by the manufacturer) at
1.5 cm (n = 3), 2.0 cm (n = 6), and 2.5 cm (n = 1).
These straight microwave antennas had a 13-gauge diameter, 15-cm length, and
3.6-cm active tip (Fig. 1).
Microwave Ablation Treat and Resect Protocol
All microwave ablations were performed intra-operatively under sonography
guidance. All operations were performed with the patient under general
anesthesia, and exposure of the targeted hepatic lobe was performed in the
standard fashion by a hepatobiliary surgical team. Intraoperative hepatic
sonography was then performed by the attending radiologist. In a systematic
manner, the location and size of the index tumor identified on preoperative CT
or MRI were reconfirmed, and the rest of the liver was scanned to ensure the
presence or absence of any other suspicious masses. The microwave antennas
were placed into the center of the index tumor under direct sonography
guidance (Fig. 2). All three
microwave generators were powered on simultaneously to achieve synchronous
ablation. All ablations were performed at a power of 45 W for a treatment
period of 10 min. Each patient underwent a single microwave ablation for their
solitary liver cancer (either HCC or CRC metastasis). Continuous sonography
monitoring was performed to track the progress of the ablation (Figs.
3A,
3B, and
3C).

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Fig. 2 Digital photograph of 48-year-old woman with colorectal
carcinoma metastases taken intraoperatively shows insertion of three single
microwave antennas (VivaWave Microwave Coagulation System, Vivant Medical)
spaced 2.0 cm apart using rigid spacer.
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Fig. 3A 48-year-old woman with colorectal carcinoma metastases
(patient 1 in Table 1).
Sequential sonograms (taken 1-2 minutes apart) show development of exuberant
transient hyperechogenic response in surrounding liver parenchyma to microwave
ablation.
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Fig. 3B 48-year-old woman with colorectal carcinoma metastases
(patient 1 in Table 1).
Sequential sonograms (taken 1-2 minutes apart) show development of exuberant
transient hyperechogenic response in surrounding liver parenchyma to microwave
ablation.
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Fig. 3C 48-year-old woman with colorectal carcinoma metastases
(patient 1 in Table 1).
Sequential sonograms (taken 1-2 minutes apart) show development of exuberant
transient hyperechogenic response in surrounding liver parenchyma to microwave
ablation.
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The extent of the ablated coagulation "front" could be roughly
approximated on the basis of the appearance of the transient hyperechoic zone.
In the case of radiofrequency ablation, the transient hyperechoic response is
said to be a rough approximation (± 8 mm) of the ablation margin
[6]. With microwave ablation,
however, the echogenic response observed was more rapid and extensive, making
visualization of the antenna and ablation zone slightly more difficult.
Therefore, response is not as useful with microwave ablation as compared with
radiofrequency ablation. Also of note was the fact that the transient
hyperechoic zone exhibited an exuberant and robust response, as previously
reported by Wright et al. [4],
thus suggesting the high intratumoral temperature achieved. Immediately after
ablation, targeted hepatic resection was completed by a surgical team. The
Pringle maneuver was not used in this study (although larger ablation volumes
would be expected with this maneuver than without this maneuver) because one
of the long-term goals of our study is to make the data set as applicable to
the percutaneous setting as possible.
Pathologic Correlation
The resected hepatic specimen, which contained the tumor and ablated
lesion, was then transported en bloc to the pathology department for immediate
processing. Specimens were inspected and measured by the pathologist. Scaled
digital photographs were taken and were later correlated with the gross
pathologic measurements to ensure the accuracy of the ablation zone size.
Representative regions of interest, which included grossly coagulated and
viable tumor, coagulated and viable liver parenchyma, and equivocal areas
within the transition zone were then frozen for further sectioning. These
sections were stained separately with the standard H and E stain and vital
histochemical nicotinamide adenine dinucleotide (NADH) stain.
In regions where H and E staining proved equivocal, staining with NADH
stain, which has an unambiguous binary staining characteristic of positive
staining indicating tissue viability and nonstaining indicating cellular
death, was used to prove or disprove tissue viability
[7]. In all cases, the primary
diagnosis of liver malignancy was confirmed by standard histologic criteria.
Tumor histology included six CRC metastases and four HCCs. Resection margins
were also scrutinized for tumor according to standard clinical protocol.
Volumetric Calculations
The approximate volumes of tumor and ablation coagulation zone were
calculated assuming an ellipsoid geometry using the following:
where V is volume, and x, y, and z represent the
diameters (in centimeters) of the three orthogonal axes.
Results
Tumor and Ablation Zone Characteristics
The mean maximal tumor diameter was 4.4 cm (range, 2.0-5.7 cm), and the
average tumor volume was 33.0 cm3 (2.3-76.3 cm3). The
mean maximal ablation diameter was 5.5 cm (5.0-6.5 cm), and the average
ablation zone volume, assuming ellipsoid geometry, was 50.8 cm3
(30.3-65.5 cm3). The measurements of the ablation zones in the
x, y, and z orthogonal planes are summarized in
Table 1. In all ablations, the
individual lesion components had completely fused to create one large
continuous ablated volume that encompassed the grossly visible tumor mass in
its entirety. Nevertheless, on closer inspection, some cross sections, those
that were perpendicular to the plane of the antenna shaft, revealed that the
ablated lesion shapes were not strictly circular but, rather, took on a
slightly triangular contour. This "deformation" was considered
minimal because no grossly apparent clefts appeared along the coagulated
border.
Histopathologic and Tumor Histochemical Characteristics
On gross inspection of the ablated zone, a central pale zone of coagulation
surrounded by a red hyperemic zone was visualized
(Fig. 4). The three microwave
antenna tracts were visualized, via careful cross sectioning, to be in the
center of each ablation volume, which in turn completely surrounded the liver
tumor.

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Fig. 4 Scaled digital photograph taken of resected gross specimen
from a 67-year-old man with colorectal carcinoma metastases (patient 6 in
Table 1) shows ablation zone
extending to hepatic vein (large arrow). Three microwave antenna
sites (small arrows) are seen in center of ablation zone. Note
central pale zone of coagulation surrounded by red hyperemic zone.
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Microscopically, on initial H and E staining, hepatocytes within the
central coagulated zone had an amorphous cytoplasm, with loss of all cellular
structure and no discernible cell membranes. Although some cells did retain
the appearance of cellular nuclei, on further examination with the vital
histochemical NADH stain for the mitochondrial enzyme NADH diaphorase
[7], no viable tissue was
seen.
Moving further from the primary (central) coagulation zone into the
surrounding zone of hyperemia, some H and E-stained areas displayed only a
subtle loss of nuclear chromatin detail with minimal cell membrane
destruction. However, using the unambiguous staining characteristic of the
histochemical NADH stain [7],
we were able to confidently discern areas of cellular viability versus areas
of cellular death at the marginall within normal liver. At the 5-mm
transition zone between grossly coagulated and clearly viable tissue, NADH
staining consistently revealed uniform cellular death with a sharp border
demarcating viable from ablated regions (Figs.
5A,
5B,
5C, and
5D).

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Fig. 5A Photomicrographs of colorectal carcinoma (CRC) metastases to
liver and of normal liver. Photomicrographs of same sections of liver from
54-year-old man (patient 2 in Table
1) with CRC metastases stained with H and E stain (A) and
vital histochemical nicotinamide adenine dinucleotide (NADH) stain (B)
show complete microwave thermocoagulation of all areas (magnification,
x100). Note this effect is more clearly seen on NADH-stained slide
(B).
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Fig. 5B Photomicrographs of colorectal carcinoma (CRC) metastases to
liver and of normal liver. Photomicrographs of same sections of liver from
54-year-old man (patient 2 in Table
1) with CRC metastases stained with H and E stain (A) and
vital histochemical nicotinamide adenine dinucleotide (NADH) stain (B)
show complete microwave thermocoagulation of all areas (magnification,
x100). Note this effect is more clearly seen on NADH-stained slide
(B).
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Fig. 5C Photomicrographs of colorectal carcinoma (CRC) metastases to
liver and of normal liver. For comparison with A and B,
photomicrographs of sections from same patient of normal liver parenchyma
obtained after microwave ablation and stained with H and E (C) and NADH
(D) stains show complete thermocoagulation on left half of slide but
viable tissue on right (magnification, x100). Note dark blue area
(viable cells) on right is more evident on NADH-stained slide (D).
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Fig. 5D Photomicrographs of colorectal carcinoma (CRC) metastases to
liver and of normal liver. For comparison with A and B,
photomicrographs of sections from same patient of normal liver parenchyma
obtained after microwave ablation and stained with H and E (C) and NADH
(D) stains show complete thermocoagulation on left half of slide but
viable tissue on right (magnification, x100). Note dark blue area
(viable cells) on right is more evident on NADH-stained slide (D).
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Large blood vessels (> 3 mm in diameter) in the resection specimens did
not create the typical ablation zone distortion that might be expected with
other thermoablative techniques due to the minimal heat sink effect observed
with microwave ablation (Fig.
6). A marked thermallike effect was observed with maximal
intensity closest to the antenna site.

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Fig. 6 Digital photograph of resected gross specimen from a
67-year-old man with colorectal carcinoma metastases (patient 8 in
Table 1) stained with
nicotinamide adenine dinucleotide (NADH) shows area of marked
thermocoagulation surrounding 4-mm hepatic vein.
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Of particular interest, in one patient who had undergone oxaliplatin
chemoembolization 1 year before microwave ablation and subsequent liver
resection, the ablated region encompassing the CRC metastasis microscopically
showed severe architectural and cellular distortion of the fibrosed and
hyalinized adenocarcinoma, more severe than any of the previous cases, with
resultant foci of barely recognizable nonviable liver and tumor tissue.
Grossly, the extent of the microwave ablation effect was also larger and more
confluent than previous CRC metastasis ablations in our series.
Complications
No direct procedural complications secondary to microwave ablation were
noted. The following complications were deemed to be temporally and
causatively related to the hepatic resection and were encountered in four
patients: non-Q wave myocardial infarction (reported surgical morbidity rate
[8], 2%; range, 1-4%), renal
failure and staphylococcal bacteremia (3%; range, 1-37%), hepatic failure
salvaged by orthotopic liver transplantation (4%; range, 0.5-28%), and
perihepatic abscess (4%; range, 1-28%) complicated by lower extremity ischemia
that resulted in eventual death (5%).
Discussion
Although resection of HCC and hepatic CRC metastases has been shown to
increase both the 5-year overall and the disease-free survival
[9-11],
many patients may have tumors that are surgically unresectable because of
either unfavorable tumor anatomy or poor patient hepatic reserve.
Radiofrequency ablation is currently the dominant thermal ablation technique
in use worldwide. Other potential thermoablative energy sources include laser,
high-intensity focused ultrasound, and microwave ablation. There are many
different strategies for applying these thermal energies including, but not
limited to, single straight electrodes, multiple expandable electrodes, pulsed
energy delivery systems, and internally cooled systems. Based on this wide
variety of choices, a substantial debate has emerged as to which of the
techniques and which of the electrode or delivery modifications are most
appropriate for specific clinical scenarios.
In addition, adequate treatment outcomes and clinical successes are often
determined by various biophysical limitations, such as the ideal tumor biology
(tumor histology, presentation, and growth rate), blood flow characteristics
(both intratumoral and surrounding the tumor), and tissue conductance. Factors
such as the local tissue composition may alter the extent of coagulation
because heat conducts differently throughout different tissue types at various
rates. Local dielectric properties can often times prove advantageous when it
results in improved (increased) heat retention during the ablations, such as
in the treatment of HCC surrounded by cirrhotic tissue
[12], lung tumors with
surrounding aerated lung [13],
and vertebral body lesions surrounded by bone cortex
[14].
Commonly reported disadvantages in the current thermoablation systems
include difficulty in treating large tumorsthat is, those exceeding 3
cm in diameter [15]; the
potential for incomplete radiofrequency tumor ablation near blood vessels
because of the heat sink effect of local blood flow
[16]; difficulty in obtaining
sonographic images of radiofrequency lesions
[17]; and evidence of
surviving tumor cells, even within radiofrequency lesions
[18]. The treatment of large
tumors can be time consuming to adequately ensure total overlapping coverage
of the ablation zones. Even with meticulous technique, tumor recurrence can be
frequent [15]. Thus, the use
of multiple electrodes to achieve larger coagulation volumes than possible
with a single electrode has been proposed.
In this regard, however, a significant difference in the physics of
microwave ablation and radiofrequency ablation should be noted. Radiofrequency
ablation involves the flow of current, in the frequency of radiowaves, within
the body tissues using conductive electrodes. Essentially, the alternating
radiofrequency current causes surrounding ions in adjacent tissue to oscillate
and collide in proportion to the intensity of the radiofrequency current. This
generates enough heat, greater than the cytotoxic threshold, thus leading to
cellular death via thermocoagulation necrosis.
Alternatively, microwave ablation generates an electromagnetic wave around
insulated, electrically independent antennas. This electromagnetic wave causes
the agitation of polar water molecules within surrounding tissue. This
vigorous movement of water molecules then raises the temperature within the
adjacent tissue causing frictional heating, thus inducing cellular death via
coagulation necrosis. Therefore, microwaves (at least theoretically) should be
more amenable than radiowaves to synchronous ablations using multiple
applicators to achieve larger tumor coagulation volumes in shorter periods of
time. Percutaneous radiofrequency ablation is currently considered the
first-line treatment for small (< 3 cm) HCC in nonsurgical candidates
[19,
20].
Microwave ablation offers many of the benefits of radiofrequency ablation
but has several theoretic advantages that may result in improved performance
near blood vessels. During radiofrequency ablation, the zone of active tissue
heating is limited to a few millimeters surrounding the active electrode, with
the remainder of the ablation zone being heated via thermal conduction
[21]. Owing to the much
broader field of power density of the electromagnetic microwave (up to 2 cm
surrounding the antenna), microwave ablation results in a much larger zone of
active heating than radiofrequency ablation
[22]. This has the potential
to allow a more uniform tumor kill in the ablation zone, both within the
targeted zone and the blood vessels next to the targeted zone. Radiofrequency
ablation is also limited by the increase in impedance with tissue boiling and
charring [23] because water
vapor and char act as electric insulators. Due to the electromagnetic nature
of the microwave, ablations performed do not seem to be subject to this
limitation, thus allowing the intratumoral temperature to be driven
considerably higher, resulting in a larger ablation zone within a shorter
ablation time period.
The use of microwave ablation, originally referred to as "microwave
coagulation therapy," has been most prevalent to date in Asia, where a
number of reported studies have shown it to be effective in the local control
of both HCC [24,
25] and metastatic CRC
[26]. The Asian system uses a
smaller microwave applicator at 2.4 GHz that creates small ablation sizes,
thereby making it difficult to treat large lesions. The new 915-MHz microwave
system that we used is more tuned to the dielectric properties of human tumor
tissue. Given this and the size of current microwave applicators, large
ablation volumes can now be achieved in fewer applications.
The initial experiments by other investigators using this new microwave
ablation system with a porcine liver model have been encouraging
[4]. Ablation volumes obtained
with simultaneous multiple straight probe ablations were significantly larger
than the same number of ablations made sequentially. In addition, these larger
volumes were obtained in the time required for a single ablation cycle, by
virtue of the simultaneous powering on of all microwave antennas. In this
preliminary clinical setting of this device in the treatment of human liver
tumors, our results appear comparable. Using a triple straight microwave
antenna configuration, we created large ablation volumes of approximately 50.8
cm3 in 10 minutes.
In addition, it is easier to target and appropriately place multiple
microwave antennas within a lesion compared with trying to place one
radiofrequency electrode in an untreated area by moving the electrode.
Subsequent placing of an additional microwave antenna 2 cm from one that is
already in place is much easier and more accurate than performing the task
without an antenna in place. Besides the synergistic use of multiple microwave
antennas in the treatment of solitary lesions, the ability to drive multiple
antennas simultaneously may be useful in the treatment of multiple tumors.
With radiofrequency ablation usually requiring between 12 and 25 minutes per
lesion, the total procedure time can be quite lengthy, especially when
attempting to treat multiple tumors. Significant time savings could be
achieved through microwave ablations with multiple antennas given the better
convection profile of microwave ablation when compared with radiofrequency
ablation.
One potential disadvantage of this triple straight antenna configuration is
the fact that ablations tended to result in a nonspherical volume, which may
have been expected given the triangular arrangement of the three microwave
antennas. Wright et al. [4]
reported in a porcine study that antenna separation of < 1.7 cm yielded
significantly rounder, more confluent-looking lesions. However, with antenna
separation of > 1.7 cm, the overall ablated lesion became less spherical.
We observed this same slight loss of border convexity in some ablation
specimen cross sections, but in all cases, the zones of coagulation had
adequately fused without spared tissue between the antennas.
Hepatic ablation is currently being used to treat and increase the number
of patients amenable to curative or palliative treatment of liver cancers
[27]. All current systems have
unique advantages and disadvantages. Cryoablation has been widely studied
intraoperatively, with higher complication rates reported when compared with
radiofrequency ablation [28].
Newer percutaneous cryotherapy systems may allow cryoablation to be used in
more patients with liver tumors. Theoretic problems with percutaneous
cryoablation include bleeding requiring additional maneuvers such as tract
coagulation with fibrin glue. Radiofrequency ablation is time consuming; is
limited to single lesions; and seems to have higher recurrence rates,
especially near blood vessels larger than 3 mm
[16]. This new microwave
ablation system currently has several theoretic advantages over radiofrequency
ablation, including an improved convection profile with consistently higher
intratumoral temperatures, larger tumor ablation volumes and faster ablation
times, and the ability to simultaneously use multiple antennas.
In conclusion, we believe this study has shown the feasibility of using
simultaneous multiple microwave antennas in the treatment of liver tumors
intraoperatively. Additional percutaneous studies are currently under way to
investigate the safety and efficacy in treating patients who are not
candidates for hepatic resection.
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