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Ovarian tissue cryopreservation for fertility preservation in 418 girls and adolescents up to 15 years of age facing highly gonadotoxic treatment. Twenty years of experience at a single center. Acta Obstet Gynecol Scand 2019; 98:630-637. [PMID: 30919447 DOI: 10.1111/aogs.13616] [Citation(s) in RCA: 39] [Impact Index Per Article: 7.8] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/19/2018] [Accepted: 03/23/2019] [Indexed: 12/21/2022]
Abstract
INTRODUCTION The preservation of fertility is an integral part of care of children requiring gonadotoxic treatments for cancer or non-malignant diseases. In France, the cryopreservation of ovarian tissue has been considered and has been offered as a clinical treatment since its inception. The aim of this study is to review 20 years of activity in fertility preservation by ovarian tissue cryopreservation (OTC) for children and the feasibility of oocyte isolation and cryopreservation from the ovarian tissue at a single center. MATERIAL AND METHODS Retrospective study including patients aged 15 years or younger who underwent OTC, combined for some with oocyte cryopreservation of isolated oocytes, before a highly gonadotoxic treatment for malignant or non-malignant disease was initiated. We describe the evolution of activities in our program for fertility preservation and patient characteristics at the time of OTC and follow up. RESULTS From April 1998 to December 2018, 418 girls and adolescents younger than 15 years of age underwent OTC, representing 40.5% of all females who have had ovarian tissue cryopreserved at our center. In all, 313 patients had malignant diseases and 105 had benign conditions. Between November 2009 and July 2013, oocytes were isolated and also cryopreserved in 50 cases. The mean age of patients was 6.9 years (range 0.3-15). The most frequent diagnoses in this cohort included neuroblastoma, acute leukemia and hemoglobinopathies; neuroblastoma being the most common diagnosis in very young patients. During follow up, three patients requested the use of their cryopreserved ovarian tissue. All had undergone ovarian tissue transplantation, one for puberty induction and the two others for restoring fertility. So far, no pregnancies have been achieved. Eighty-four patients who had OTC died. CONCLUSIONS Ovarian tissue cryopreservation is the only available technique for preserving fertility of girls. To our knowledge this is the largest series of girls and adolescents younger than 15 years so far reported on procedures of OTC before highly gonadotoxic treatment in a single center.
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Testicular transposition in children undergoing brachytherapy for bladder and/or prostate rhabdomyosarcoma. J Pediatr Surg 2018; 53:1428-1431. [PMID: 29753523 DOI: 10.1016/j.jpedsurg.2018.04.018] [Citation(s) in RCA: 10] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 12/22/2017] [Revised: 04/04/2018] [Accepted: 04/08/2018] [Indexed: 11/27/2022]
Abstract
BACKGROUND/PURPOSE Fertility preservation is a major goal in treatment of children with cancer. We describe a new technique of testicular transposition (TT) in patients treated with pulse-dose-rate (PDR) brachytherapy as part of the multimodal conservative treatment of bladder neck and/or prostate rhabdomyosarcoma (BP RMS). METHODS Medical records of consecutive patients treated between September 2016 and August 2017 were studied. These patients underwent a TT performed during BP RMS surgery by the same suprapubic incision. The external oblique aponeurosis was not incised. The spermatic cord was mobilized up to the external inguinal ring, and the gubernaculum attachments were severed from the scrotum. The testis was then flipped over with care taken to avoid injury of the vessels or the vas, wrapped in a silicone material and sutured under the abdominal skin with a transfixing stitch facing the anterior superior iliac spine. At the end of brachytherapy, the testis was relocated in the scrotum and during the same general anesthesia, plastic tubes and stents were removed. Surgical outcome and dosimetric parameters were examined. RESULTS Eight patients were identified. Median age was 24 months (range 11-80 months). All had embryonal BP RMS and received chemotherapy according to RMS 2005 protocol prior to local treatment. All patients underwent conservative surgery followed by brachytherapy (60 Gy) and had testicular transposition of one testis. None had surgical complications. After converting doses to biologically equivalent doses in 2-Gy fractions (EQD2), the dose delivered to 75% of the transposed testis was 1.5 GyEQD2 (1-3 GyEQD2), versus 5.4 GyEQD2 (3.9-9.4 Gy EQD2) for the untransposed testis (p < 0.001). CONCLUSION Testicular transposition is feasible in order to potentially preserve fertility and future quality of life in children undergoing brachytherapy for BP RMS. TYPE OF STUDY Level IV Treatment Study: Case Study with no Comparison Group.
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Abstract
Installation of a modern high-energy Siemens Primus linear accelerator at the Northern Centre for Cancer Treatment (NCCT) provided the opportunity to investigate the optimal clinical implementation of the Siemens virtual wedge filter. Previously published work has concentrated on the production of virtual wedge angles at 15 degrees, 30 degrees, 45 degrees, and 60 degrees as replacements for the Siemens hard wedges of the same nominal angles. However, treatment plan optimization of the dose distribution can be achieved with the Primus, as its control software permits the selection of any virtual wedge angle from 15 degrees to 60 degrees in increments of 1 degrees. The same result can also be produced from a combination of open and 60 degrees wedged fields. Helax-TMS models both of these modes of virtual wedge delivery by the wedge angle and the wedge fraction methods respectively. This paper describes results of timing studies in the planning of optimized patient dose distributions by both methods and in the subsequent treatment delivery procedures. Employment of the wedge fraction method results in the delivery of small numbers of monitor units to the beam's central axis; therefore, wedge profile stability and delivered dose with low numbers of monitor units were also investigated. The wedge fraction was proven to be the most efficient method when the time taken for both planning and treatment delivery were taken into consideration, and is now used exclusively for virtual wedge treatment delivery in Newcastle. It has also been shown that there are no unfavorable dosimetric consequences from its practical implementation.
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Validation of treatment planning system data: variation in the modelling of three 6 MV beams for extreme rectangular fields. Radiother Oncol 2001; 60:329-32. [PMID: 11514013 DOI: 10.1016/s0167-8140(01)00385-1] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/23/2022]
Abstract
The validation of photon beam data on the Helax-TMS treatment planning system at the Northern Centre for Cancer Treatment takes the form of profile and depth dose comparisons against measured data for square fields. With a view to using Helax-TMS to plan fixed source-to-surface distance spine fields, validation of extreme rectangular fields was undertaken, based on guidelines published by the American Association of Physicists in Medicine Radiation Therapy Committee (Task Group report 53). The accuracy with which the Helax-TMS-generated profiles matched those measured varied between treatment machines. For three 6 MV beams in the department, two beams showed agreement to within 2% in the central portion of the field, while the third beam demonstrated differences of up to 4.4% in this region. The disparities were attributed to the modelling of the primary dose for each beam by Helax-TMS.
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Abstract
BACKGROUND AND PURPOSE This paper describes a practical method of elevating the surface dose of clinical electron beams in the energy range 3-12 MeV using thin high density metal foils (tin and lead) as an alternative to tissue equivalent bolus. Because, relative to water, these materials exhibit a high scattering power to stopping power ratio, the desired dose elevation may be achieved with less energy loss than conventional bolus and consequently a gain in therapeutic interval. METHODS The foil thickness required to raise the surface dose to 90% off peak, for a given electron energy, was calculated using published scattering and stopping power data. An empirical expression is derived to facilitate calculation of foil thickness (tin or lead) to produce a given surface dose. RESULTS AND CONCLUSIONS Measurements were made to confirm the predictions of the derived expression and were found to be in good agreement.
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Spectral estimation and contrast calculation in the design of contrast-detail test objects for radiotherapy portal imaging. Phys Med Biol 1999. [DOI: 10.1088/0031-9155/38/4/006] [Citation(s) in RCA: 9] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
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Abstract
Lithium fluoride (TLD-700) dosimeters were used to measure exit surface absorbed doses in external beam radiotherapy using an automated TLD reader. Delivered tumour absorbed doses were derived from these measurements for head and neck, pelvis and breast treatments. For the head and neck treatments (first fraction only), the mean percentage difference between prescribed and delivered tumour absorbed doses was -0.15 +/- 3.0% (+/- 1 SD), for the pelvic treatments -0.83 +/- 2.8% and for the breast treatments +0.26 +/- 2.9%. The spread of results is approximately +/- 3% (+/- 1 SD). This is comparable with the estimated uncertainty in a single TLD absorbed dose measurement in phantom (+/- 2%; +/- 1 SD). Thus, ICRU recommended tolerances for absorbed dose delivery of +/- 5% may not be unequivocally detectable using this method. An action level of +/- 10% is suggested, allowing investigation of possible gross errors in treatment delivery at an early stage, before the course of treatment has progressed to a point at which absorbed dose compensation is impossible.
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Abstract
We have measured plasma and cerebrospinal fluid (CSF) concentrations of nociceptin, the endogenous agonist of the orphan opioid receptor-like receptor (ORL-1). We studied two groups of ten patients presenting for elective Caesarean section (Group E) or in established labour and requiring combined spinal epidural anaesthesia for pain relief (Group L). Nociceptin was identified in all CSF samples with mean +/- SD concentrations of 52.49 +/- 34.25 and 63.39 +/- 33.26 pg/ml in groups E and L, respectively. Nociceptin was identified in 16/20 plasma samples with mean +/- SD concentrations of 7.59 +/- 21.58 and 13 73 +/- 23.79 pg/ml in groups E and L, respectively. CSF concentrations were significantly higher than plasma concentrations and there were no differences between groups E and L. These data report the first measurements of CSF nociceptin in man and show no association with the acute pain of labour.
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Automated TLD system for tumor dose estimation from exit dose measurements in external beam radiotherapy. Int J Radiat Oncol Biol Phys 1997; 38:899-905. [PMID: 9240660 DOI: 10.1016/s0360-3016(97)00282-4] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/04/2023]
Abstract
PURPOSE An automated TLD facility has been commissioned and calibrated, and techniques have been developed for the measurement of exit doses in external beam radiotherapy, to enable the routine estimation of delivered tumor doses. METHODS AND MATERIALS An automated TLD system, originally intended for use in diagnostic radiology and radiation protection, has been evaluated and configured for the measurement of exit doses in radiotherapy. Linearity, optimum heating cycles and calibration procedures have been determined. At the photon energies used, encapsulated lithium fluoride chips provide insufficient buildup to ensure electronic equilibrium, necessitating calibration to allow for oblique exit surfaces. Expressions are derived to allow the calculation of delivered tumor doses. RESULTS Under the calibration conditions described, the uncertainty in a single TLD measurement is approximately +/-2% (+/-1 standard deviation). Over the dose range 0.4-1.5 Gy, TL response is linear. The total heating cycle time, including annealing, is 75 s. Measurements of R(exit) (the ratio of exit dose with and without full backscatter), used in the estimation of tumor doses, decreases with field size for small fields and varies only slightly for field sizes greater than 7 x 7 cm. Lack of electronic equilibrium leads to a decrease in R(exit) with increasing exit surface obliquity for all energies considered. Application of the technique to a simulated treatment showed good agreement between estimated and applied tumor doses, when surface obliquity was taken into account. CONCLUSION This work describes the commissioning and calibration of an automated TLD facility and demonstrates that exit surface measurements using TLD chips used under conditions where electronic equilibrium was not established, have the potential for identifying discrepancies in delivered tumor doses.
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Abstract
A method is presented for matching wedge field dose distributions on different treatment units, simplifying the transfer of patients between machines during machine failure or scheduled downtime and avoiding the need for a full re-plan in most cases. Differences in wedge field characteristics between machines are accounted for and differences in energy are easily accommodated.
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A method and contrast-detail phantom for the quantitative assessment of radiotherapy portal imaging systems. Br J Radiol 1994; 67:384-8. [PMID: 8173880 DOI: 10.1259/0007-1285-67-796-384] [Citation(s) in RCA: 7] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/29/2023] Open
Abstract
Several designs of electronic portal imaging systems for radiotherapy have been reported or are now commercially available, as well as the familiar radiographic screen-film combinations. In order to evaluate imaging performance of these, and future, systems a prototype contrast-detail test object has been developed in conjunction with a method for determining contrast from a model of the X-ray spectra produced by linear accelerators. Several existing test objects rely on qualitative or semi-quantitative estimates of contrast. In this technique, quantitative estimates of contrast may be determined for each detail size from realistic estimates of the X-ray spectrum by using a spectral model either in conjunction with narrow-beam attenuation measurements on the linear accelerator used, or by using the nominal value of maximum photon energy. This technique should facilitate the comparison of imaging systems used with linear accelerators of different energies as well as providing a quantitative quality control tool for regular measurements of imaging performance. Examples of the use of the test object in the evaluation of several commercial screen-film combinations are given.
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Abstract
In photon beam therapy, the geometric penumbra width is determined by the source-size and the collimator design. The width of the physical (i.e. dosimetric) penumbra involves an additional contribution from secondary electron spread. Using a suitably defined measure of penumbra width, the separate widths due to photons and secondary electrons are additive in quadrature. Secondary electron spread functions were measured using photographic dosimetry for 60Co gamma rays and for 4, 8 and 16 MV X rays. The results suggest that, under typical treatment conditions, secondary electron spread may be the predominant contributor to the penumbra at effective generating voltages exceeding 10 MV. The implications for selection of beam energy in precision small-field radiotherapy are discussed briefly.
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Results of treatment of carcinoma of the uterine cervix using the Newcastle afterloading technique. Br J Radiol 1989; 62:64-7. [PMID: 2914193 DOI: 10.1259/0007-1285-62-733-64] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/03/2023] Open
Abstract
Eighty-seven patients with carcinoma of the uterine cervix were seen between 1 August 1977 and 31 December 1985. Seventy-one patients were treated radically. A combination of intracavitary radiotherapy, using the Newcastle manual afterloading technique, and external-beam radiotherapy was used. The actuarial 4-year survival for all Stage 1 cervical carcinomas was 84.9%. For Stage 2 cancers the actuarial local control rate was 71.1% and the survival 49.2% and for Stage 3 cancers the 4-year actuarial local control rate was 24.3% and the survival 14.8%. Complications of treatment were confined to the bowel and bladder and occurred in 11.5% of cases. The results of treatment of Stage 1 cancer suggest that the intracavitary technique gives a satisfactory distribution of radiation. The results of treatment of more advanced cases are disappointing and suggest that improvements are possible for some patients (i.e. wedge malalignment patients). There is sufficient flexibility in the technique for it to be applied satisfactorily for most anatomical situations.
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Abstract
The Manchester method of gynaecological treatment using radium 226, ovoids and a flexible intrauterine tube has been used in many centres. In Newcastle, the Manchester technique was used until 1971, when a manually afterloaded system (MAS) using caesium 137 and two source trains was introduced. In 1985, the MAS was replaced by the Selectron remote afterloading system (RAS), which also uses caesium-137 sources. The dosimetry of this remote system has been designed to produce the same shape of isodose distributions as the MAS, but shorter treatment times. The applicator design and the dosimetry of the system used in Newcastle are discussed. Dose rates achieved by the RAS are more than double those currently produced by the MAS, and a reduction in prescribed dose of 10-20% is being made. The percentage of ward staff receiving monthly doses of more than 0.2 mSv has fallen from 78% to 18% since the introduction of the remote afterloading system. The almost-cylindrical isodose distributions facilitate matching of external beam treatments using a central lead wedge to the intracavitary treatments, and work is in progress to develop this technique.
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A radiographic test object for the LDR Selectron remote afterloading system. Br J Radiol 1988; 61:637-8. [PMID: 3408853 DOI: 10.1259/0007-1285-61-727-637] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/05/2023] Open
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Abstract
An applicator attached to a 6 MV linear accelerator has been adapted to produce a well defined beam for the treatment of retinoblastoma. By using a contact lens as the reference point on the patient's cornea, the beam edge is aligned to just behind the posterior margin of the crystalline lens, thus sparing the anterior chamber and lens from the radiation field. In addition to basic dosimetric measurements made using an ionisation chamber and film densitometry to quantify the output and dose distribution from the applicator, extensive use was made of thermoluminescent dosemeters and a tissue-equivalent anthropomorphic head phantom. This was designed for detailed dosimetry on the eye and was used to confirm the correct positioning and reproducibility of the clinical set-up. We present data that corroborate and extend the dosimetric analyses documented in an earlier Dutch publication. In addition to the improved dosimetric analysis, other advantages include patient immobilisation, anaesthetic procedure and finer couch control as well as a recommendation on the dose prescription.
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Abstract
The total-body irradiation (TBI) technique at St Bartholomew's Hospital has been developed to improve dose homogeneity within the patient. Using a standard 6 MV linear accelerator in an orthodox-sized treatment room, the midpoint doses in head, neck, shoulders, mid-mediastinum, pelvis, knees and ankles are +/- 5% of that of the umbilicus in our current technique. This homogeneity has been achieved by a four-field technique, a reproducible patient set-up, careful use of a new bolus material and an additional beam-flattening filter mounted near the machine head. In addition, thermoluminescent dosimetric data collected at a test irradiation before TBI are used to influence field weightings and further improve dosimetry. This individualised and empirical TBI technique has dosimetric advantages over theoretical TBI dosimetric considerations in reducing dose gradients within the patient. These advantages are discussed.
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Unforeseen variation of electron output with field size following modification of linear accelerator treatment head. Br J Radiol 1985; 58:1229-30. [PMID: 3842639 DOI: 10.1259/0007-1285-58-696-1229-b] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/07/2023] Open
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Combining backscattered electrons and low energy photons to improve the dose distribution to an eyelid. Int J Radiat Oncol Biol Phys 1985; 11:617-20. [PMID: 3972671 DOI: 10.1016/0360-3016(85)90197-x] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/08/2023]
Abstract
In electron beam therapy, backscattered electrons from metal shields result in a high dose to tissue in the vicinity of the shield. Data are now available which enable both the magnitude of the dose enhancement at the interface and the fall off in dose 'up stream' to be determined. With the aid of these data, a combined modality therapy (5 MeV electrons, 1.1 mm A1 HVL X rays) was given to an eyelid during which the lens was protected with a superficial X ray lead eye shield. The eyelid was treated to a mid lid dose of 45 Gy in 28 days, and the dose gradient on the beam central axis was more uniform (+/- 3%) than that obtainable with superficial X rays alone. The lens dose from the combined therapy was estimated to be less than 0.25 Gy.
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Abstract
A coin-shaped ionisation chamber, orientated with its thin window facing away from the radiation source, was used to investigate the dose perturbations caused by the absence of back-scattering material near the exit surface of solid phantoms. Cobalt 60 and 4, 8 and 16 MV X-ray beams were used in the study. With no scattering material beyond the chamber window the ionisation was found to be as much as 17% less than the full scatter value. This was attributed to the absence of both back-scattered electrons and back-scattered photons. Full electron back-scattering could be restored by placing between 1.0 and 2.7 mm of unit density material beyond the chamber, depending on the primary beam energy. Under these circumstances the reduction in dose, now due to the absence of back-scattered photons only, was found to be small.
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Abstract
Whenever a heterogeneity is present in an electron beam treatment field during radiotherapy, there is the possibility of tissue overdosage at the tissue-heterogeneity interface due to electrons backscattered from the heterogeneity. Measurements of this effect were made in a polystyrene phantom using a purpose-built thin-window parallel-plane ionisation chamber. Materials of various atomic numbers were used as scatterers and the investigations were made over a wide range of electron energies. Electron backscatter factor (EBF), defined as the ratio fo dose at the interface surface with and without the scatterer present, was found to increase with increasing atomic number and decrease with increasing beam energy. Both of these relationships were found to be non-linear. The EBF dependence on the scatterer thickness was also investigated. All data in this work were expressed in relation to the beam energy incident on the scatterer in preference to the nominal beam energy set on the accelerator. This approach enables the dose enhancement at an interface to be predicted from a knowledge of the heterogeneity (atomic number and thickness,), its depth in tissue and the beam energy being used for treatment. The results of this work were compared with the published data and an explanation is offered to account for the difference.
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