

ORIGINAL ARTICLE 



Year : 2016  Volume
: 41
 Issue : 2  Page : 129134 

Determination of optimal number of beams in direct machine parameter optimizationbased intensity modulated radiotherapy for head and neck cases
Vaitheeswaran Ranganathan^{1}, KJ Maria Das^{2}
^{1} Philips Radiation Oncology Systems, Philips Ltd., Bengaluru, Karnataka; Research and Development Center, Bharathiar University, Coimbatore, Tamil Nadu, India ^{2} Department of Radiotherapy, Sanjay Gandhi Post Graduate Institute of Medical Sciences, Lucknow, Uttar Pradesh, India
Date of Submission  06Jan2016 
Date of Decision  25Mar2016 
Date of Acceptance  27Mar2016 
Date of Web Publication  3May2016 
Correspondence Address: K J Maria Das Department of Radiotherapy, Sanjay Gandhi Post Graduate Institute of Medical Sciences, Lucknow, Uttar Pradesh India
Source of Support: None, Conflict of Interest: None  Check 
DOI: 10.4103/09716203.181633
Abstract   
This paper aims to introduce an algorithm called &##8220;sensitivitybased beam number selection (SBBNS)” for fully automated and casespecific determination of an optimal number of equispaced beams in intensitymodulated radiotherapy (IMRT). We tested the algorithm in five head and neck cases of varying complexity. We used direct machine parameter optimization method coupled with Auto Plan feature available in Pinnacle TPS (Version 9.10.0) for optimization. The Pearson correlation test shows a correlation of 0.88 between predicted and actual optimal number of beams, which indicates that SBBNS method is capable of predicting optimal number of beams for head and neck cases with reasonable accuracy. The major advantage of the algorithm is that it intrinsically takes into account various case and machinespecific factors for the determination of optimal number. The study demonstrates that the algorithm can be effectively applied to IMRT scenarios to determine case specific and optimal number of beams for head and neck cases.
Keywords: Dose to organs at risk; inverse planning in intensitymodulated radiotherapy; Linac radiotherapy; orientation of radiotherapy beams
How to cite this article: Ranganathan V, Maria Das K J. Determination of optimal number of beams in direct machine parameter optimizationbased intensity modulated radiotherapy for head and neck cases. J Med Phys 2016;41:12934 
How to cite this URL: Ranganathan V, Maria Das K J. Determination of optimal number of beams in direct machine parameter optimizationbased intensity modulated radiotherapy for head and neck cases. J Med Phys [serial online] 2016 [cited 2020 Oct 19];41:12934. Available from: https://www.jmp.org.in/text.asp?2016/41/2/129/181633 
Introduction   
The selection of optimal number of beams has been of interest since the advent of 3D conformal radiation therapy. Currently, the beam number selection (BNS) process in intensitymodulated radiotherapy (IMRT) is based on the experience of the treatment planners or by a trialanderror approach. Over the past decade, many researchers have attempted to automate the beam placement process in IMRT. It is well established that optimization of beam angles in IMRT is useful in generating better treatment plans.^{[1],[2]} Currently, there exist a number of beam angle optimization (BAO) algorithms which give casespecific solution to the beam angle problem.^{[3],[4],[5],[6],[7],[8]} However, the use of BAO algorithm in routine clinical practice is not yet widespread. Many clinics still adopt the method of placing a sufficient number of equispaced beams, which has been found to produce clinically acceptable dose distribution in many anatomic sites such as head and neck. However, research has shown that manual specification of a number of equispaced beams, which is faroff from the optimal value, can either affect the plan's quality or its delivery efficiency.^{[9],[10]} This result has triggered attempts to determine an appropriate number of equispaced beams in IMRT either by studying the effect of beam numbers in the quality of IMRT plan ^{[11],[12]} or by approaching the problem from fundamental theoretical viewpoints.^{[13],[14]}
One common observation from these studies is that the optimal number of beams that strike a correct balance between plan quality and delivery efficiency is highly dependent on the case complexity. However, till date, user does not have a systematic and casespecific way to choose the number of equispaced beams in IMRT, thereby increasing interuser variability in plan quality. Moreover, in complex clinical situations, it is not easy to decide an appropriate number of beams without many trialanderror approaches potentially involving some backtracking steps. Apart from being an independent problem, BNS has also become an important step before optimizing the beam angles because many of the current BAO algorithms require the input of an appropriate number of beams for a given plan.
Our motivation is to arrive at a systematic method for determining the number of beams so that a computer program can be used to automatically determine the number of beams within a reasonable amount of time. To this end, we propose an algorithm for fully automated and casespecific selection of optimal number of beams in IMRT.
Materials and Methods   
Sensitivitybased beam number selection
In singlecriteria optimization, composite objective function is an overall estimate of the plan quality. A smaller value of the objective function is an indication of better plan quality. In this work, first, we experimentally show that the sensitivity of organ's atrisk (OAR) objective function to the prescribed target minimum dose is inversely proportional to the total number of beams. This behavior is exploited in the proposed algorithm for BNS. We term this approach sensitivitybased BNS (SBBNS), the patent application of which can be found here.^{[15]} If less number of beams are used, composite objective function of OAR objectives will be more sensitive to an increase in the target minimum dose whereas if more number of beams are used, composite objective function of OAR objectives will be less sensitive to an increase in the target minimum dose. In other words, the objective sensitivity of OAR objectives is inversely proportional to the number of beams used in the plan. SBBNS algorithm uses this behavior for predicting optimal beam number as described in the following sections. To invoke SBBNS algorithm, the user is required to set up a reference condition for each case. The reference condition mainly involves as follows:
 An equispaced beam geometry as specified in equation 1
 The number of equispaced beams would be seven in all the cases.
[Table 1] lists the other reference conditions to be adopted before invoking SBBNS algorithm. Seven beams are used in the reference condition as it allows sampling a good portion of the target volume and other normal organs over 360° rotation. Moreover, seven beams in a plan do not prolong the dose calculation and optimization significantly.  Table 1: A list of reference conditions adopted while calculating beam number constant (k)
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The beam angles in equispaced beam geometry are given by
where θ_{i} is the gantry angle of beam i, N is the number of beams, and θ_{1} is the starting gantry angle or gantry angle of the first beam.
Once the reference conditions are set, now the user can invoke the algorithm for BNS. The algorithm essentially involves two steps:
Step 1: SBBNS algorithm takes as input the clinical dosevolume objectives and calculates the objective sensitivity with respect to a predefined change in the prescribed target dose.
Step 2: The estimated sensitivity of the objective function is used to calculate optimal beam number for the given case.
A detailed account on steps 1 and 2 is given below:
Step 1: Computation of objective sensitivity
SBBNS algorithm is implemented on the following quadratic dosevolume based objective function given by:
where r represents the r ^{th} objective function component (OFC), D_{r}and V_{r} represent the dose and volume parameters for the r ^{th} OFC, respectively, and W_{r} is the importance or penalty factor for the r ^{th} OFC. f (D_{r}, V_{r}) is the numerical value of the r ^{th} OFC.
Essentially, an OFC represents a quadratic difference between userspecified clinical goal and obtained dose at each voxel multiplied by the importance factor assigned to the voxel belonging to a region of interest. In the SBBNS method, we define D_{r}and V_{r} as the clinical goal (i.e. the &##8220;real objective”) for the r ^{th} objective component.
We selected target minimum dose objective (in Auto Plan) of the planning target volume (PTV) as the reference to gauge the sensitivity of objective function. The following steps are used to determine the sensitivity of objective function:
 The direct machine parameter optimization (DMPO) plan is first optimized using the initial parameters D_{r}, V_{r}, and W_{r} to obtain the objective function F_{normal}. The plan obtained in this stage is plan A
 The second DMPO plan is generated in which the target dose of the PTV is made more stringent than the prescription goal for the PTV. For example, if the prescription requires only 95% of the PTV to receive a 6300 cGy dose, the second DMPO plan might be generated by requiring 95% of the PTV to receive 6800 cGy. The current plan is optimized, and the objective function obtained in this step is denoted as F_{overconstrained}. The plan obtained in this stage is plan B
 The objective sensitivity (S) is measured by the change in the composite objective function of all OAR objectives included in the optimization between plan A and plan B obtained for a unit objective weight (W) given by
The square root function is used because DMPO objective function is essentially a quadratic function over dose and volume parameters. Here, l is a linearization factor applied to linearize the numerator value, whose value is decided based on F_{normal}. The value of l is decided in such a way that falls in between 0.1 and 1. The same linearization factor will be applied to F_{overconstrained} term as shown in equation 3. For instance, if F_{normal} is 0.x, l is set to 1; if F_{normal} is x, l is set to 10; if F_{normal} is 0.00x, l is set to 0.01; if F_{normal} is x00, l is set to 1000, and so on. Here, x denotes an arbitrary integer.
Essentially, the sensitivity of objective function (equation 3) measures how much the objectives of surrounding critical normal structures are compromised for any change in the prescribed PTV (target) dose. The overconstraining of target minimum dose results in sacrificing the sparing of other structures, as a result of which, F_{overconstrained} is always greater than F_{normal}. Such sensitivitybased approaches had been used earlier for automated determination of IMRT objective function parameters ^{[16],[17]} and selection of optimal beam angles in IMRT.^{[18]} We verified the relationship between objective sensitivity and number of beams in a chosen head and neck anatomy as shown in [Figure 1]. It is clear from this figure that the objective sensitivity is inversely proportional to the number of beams.  Figure 1: The plot of sensitivity of objective function with respect to a 500 cGy increment in the prescribed target dose corresponding to beam numbers 3–11 for a reference head and neck case
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Step 2: Determination of optimal beam number (Step 2)
It is evident from [Figure 1] that the OAR objective sensitivity will be lower for a given case if there is enough number of beams to ensure the normal tissue sparing when prescribed target dose is increased as mentioned before. Similarly, the OAR objective sensitivity will be higher for the same case if there is not enough number of beams to ensure the normal tissue sparing when prescribed target dose is increased. Stated differently, if the objective sensitivity is found to be higher, the number of beams required to produce an optimal dose distribution for target volume and OARs would be more. Hence, the required number of beams for a given case is proportional to the sensitivity of the objective function obtained under the reference beam geometry condition. Let N_{optimal} be the optimal number of beams for a given case, then
N_{optimal} = k.S(4)
where k is a beam number constant, which is calculated under reference beam geometry condition using a reference case for which the optimal beam number is known. By manipulating equation 4, one can obtain k as given below:
where denotes the known optimal beam number for a reference case under reference beam geometry condition.
In this work, we chose a moderately complex head and neck case as a reference and applied the reference conditions mentioned before to calculate beam number constant k. To find out N_{optimal} for this case, objective function saturation curve is plotted [Figure 2]a for different beam numbers starting from 3 to 11 and an optimal beam number is chosen for the reference case. From [Figure 2]a, it is evident that at beam number seven the objective function approximately saturates. Meanwhile, S was calculated for this case as explained in step 1.  Figure 2: Objective function saturation curves obtained for head and neck  reference case (a), head and neck  Case 1 (b), head and neck  Case 2 (c), head and neck  Case 3 (d), head and neck  Case 4 (e) and head and neck  Case 5, (f) corresponding to beam numbers 3–11
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By substituting these values in equation 5, one can get the value of beam number constant (k) as below:
Using the above value of k in equation 4, it gives the optimal number of beams.
N_{optimal}= 18.32.S(7)
Equation 7 gives the final expression for the optimal beam number required regarding sensitivity of the objective function (S) obtained for a given head and neck case using equation 3. The whole process involved in SBBNS algorithm is illustrated in [Figure 3].  Figure 3: The flowchart of sensitivitybased beam number selection algorithm
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Results   
We used five head and neck cases for which optimal number of beams is to be found. The cases chosen in the study have a wide range of complexity in terms of tumor geometry, normal tissue locations, and dose and dosevolume objectives. [Table 2] gives the typical clinical objectives for the head and neck cases. To validate the proposed algorithm, we independently determined the optimal number of beams for all the five cases using objective function saturation curves. An objective function saturation curve is a graphical illustration of how the composite objective function changes with respect to a number of equispaced beams (3–11 equispaced beams) used in the optimization for the same clinical objectives set for PTVs and OARs. In the saturation curve, the optimal beam number is chosen to be the point (in the graph) at which the objective function has approximately started to saturate. We considered the starting point of the saturation as optimal because adding more beams in the optimization beyond the saturation point has been found to be only increasing the total monitor unit (MU) of the plan without improving the plan quality.^{[10]} Quantitatively, the saturation point is considered to be a beam number (in the saturation plot) beyond which the reduction in composite objective value is not more than 10%.  Table 2: Typical dosevolume objectives used in the Auto Plan module of Pinnacle for the head and neck cases. The total number of fractions was 35
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We used Auto Plan feature available in Pinnacle TPS Version 9.10.0 (Philips Radiation Oncology Systems, Fitchburg, WI) for all the DMPO optimizations, which automatically sets appropriate objective function parameters (dose, volume, and weight) for each objective. The number of segments input to DMPO algorithm before optimization was set as sixty in all the optimizations involving different equispaced beam numbers. [Figure 2]a,[Figure 2]b,[Figure 2]c,[Figure 2]d,[Figure 2]e,[Figure 2]f show the objective function saturation curves obtained for the head and neck cases. As mentioned earlier, the optimal beam numbers for each case is located by taking input from the saturation curves. At the same time, we used the proposed SBBNS algorithm to find the optimal beam number for the same cases using equation 7. [Table 3] compares the optimal number of beams obtained using the saturations curves and the proposed SBBNS algorithm. We rounded off the number predicted by SBBNS to nearest whole number. It is evident from [Table 3] that the beam number predicted using SBBNS and saturation curves are in complete agreement for three cases (case 1, 3, and 5). SBBNS has predicted two additional beams for Case 2 and one additional beam for Case 4. The Pearson correlation test shows a correlation of about 0.9 between S and N_{optimal}(obtained from saturation curves) and a correlation of about 0.88 between N_{optimal}(obtained from saturation curves) and N_{optimal}(computed using equation 7). This result indicates that SBBNS method is capable of predicting optimal number of beams for head and neck cases with reasonable accuracy.  Table 3: The comparison of optimal beam numbers obtained using objective function saturation curves and sensitivitybased beam number selection algorithm
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Discussion   
Producing a good dose distribution fundamentally requires an appropriate selection of a number of beams and their angles. It has been reported that adding more beams in IMRT beyond a point increases the MUs without any considerable improvement in dose distribution, leading to more leakage radiation, and increased critical organ dose.^{[10],[11]} At the same time, having an insufficient number of beams can result in suboptimal treatment plan. Hence, determining a suitable beam number turns out to be a valid clinical problem that requires a casespecific solution.
It is to be noted that the beam numbers determined using SBBNS algorithm are tightly coupled with the user defined objectives. Inputting simple and easily achievable objectives in SBBNS will result in a relatively lesser number of beams. Likewise, inputting complex objectives will result in a larger number of beams. Hence, it is important to ensure that the clinical objectives included in the optimization are reasonable and clinically relevant to fully make use of SBBNS approach for BNS.
Auto Plan has been used just as a substitute to an expert planner in this study. In the absence of Auto Plan feature, a planner has to decide the objective function parameters to meet the clinical objectives. The clinical validation of Auto Plan can be found elsewhere.^{[19],[20]} Moreover, the proposed SBBNS approach coupled with autocontouring tools such as SPICE and automatic planning tools such as Auto Plan allows for a complete automation of the planning process once the clinical objectives are set.
The susceptibility of beam number constant value (k = 18.32) to any change in the reference conditions mentioned in [Table 1] needs to be investigated. For instance, it will be useful to see how kvalue changes if the starting angle is set as a nonzero angle. However, a huge change in k is not expected because the numerator of beam number constant term (equation 6) will change correspondingly to any change in the denominator term occurring due to alterations in the reference conditions.
Conclusion   
It is evident from the results that the algorithm is capable of predicting optimal beam number with reasonable accuracy. Although we included only head and neck geometry in this study, in theory, the method should also be applicable to other anatomic sites such as thorax and pelvis. However, a detailed investigation might be required to understand how the proposed beam number constant value changes according to anatomy.
Financial support and sponsorship
Nil.
Conflicts of interest
There are no conflicts of interest.
References   
1.  Rowbottom CG, Webb S, Oldham M. Improvements in prostate radiotherapy from the customization of beam directions. Med Phys 1998;25(7 Pt 1):11719. 
2.  Schreibmann E, Xing L. Feasibility study of beam orientation classsolutions for prostate IMRT. Med Phys 2004;31:286370. 
3.  Pugachev B, Boyer AL, Xing L. Beam orientation optimization in intensitymodulated radiation treatment planning. Med Phys 2000;27:123846. 
4.  Hou Q, Wang J, Chen Y, Galvin JM. Beam orientation optimization for IMRT by a hybrid method of the genetic algorithm and the simulated dynamics. Med Phys 2003;30:23607. 
5.  Gaede S, Rasmussen H, Wong E. An algorithm for systematic selection of beam directions for IMRT. Med Phys 2004;31:37688. 
6.  Pugachev A, Boyer AL, Xing L. Beam orientation optimization in intensitymodulated radiation treatment planning. Med Phys 2000;27:123845. 
7.  Wu X, Zhu Y. A mixedencoding genetic algorithm with beam constraint for conformal radiotherapy treatment planning. Med Phys 2000;27:250816. 
8.  Li Y, Yao J, Yao D. Automatic beam angle selection in IMRT planning using genetic algorithm. Phys Med Biol 2004;49:191532. 
9.  Stein J, Mohan R, Wang XH, Bortfeld T, Wu Q, Preiser K, et al. Number and orientations of beams in intensitymodulated radiation treatments. Med Phys 1997;24:14960. 
10.  Narayanan VK, Vaitheeswaran R, Bhangle JR, Basu S, Maiya V, Zade B. An experimental investigation on the effect of beam angle optimization on the reduction of beam numbers in IMRT of head and neck tumors. J Appl Clin Med Phys 2012;13:3912. 
11.  Popple RA, Fiveash JB, Brezovich IA. Effect of beam number on organatrisk sparing in dynamic multileaf collimator delivery of intensity modulated radiation therapy. Med Phys 2007;34:37529. 
12.  Söderström S, Brahme A. Which is the most suitable number of photon beam portals in coplanar radiation therapy? Int J Radiat Oncol Biol Phys 1995;33:1519. 
13.  Bortfeld T. The number of beams in IMRT – Theoretical investigations and implications for singlearc IMRT. Phys Med Biol 2010;55:8397. 
14.  Fenwick JD, PardoMontero J. Numbers of beam angles required for nearoptimal IMRT: Theoretical limits and numerical studies. Med Phys 2011;38:451830. 
15.  Ranganathan V, Ranjan US. Apparatus for Determining a Number of Beams in IMRT. United States patent application, 2014; US 14/763539. 
16.  Zhang X, Wang X, Dong L, Liu H, Mohan R. A sensitivityguided algorithm for automated determination of IMRT objective function parameters. Med Phys 2006;33:293544. 
17.  Vaitheeswaran R, Narayanan VS, Bhangle J, Nirhali A. TUABRA05: An algorithm for automated determination of IMRT objective function parameters. Med Phys 2010;37:3369. 
18.  Vaitheeswaran R, Narayanan VK, Bhangle JR, Nirhali A, Kumar N, Basu S, et al. An algorithm for fast beam angle selection in intensity modulated radiotherapy. Med Phys 2010;37:644352. 
19.  Jeong K, Bzdusek K, Kumar P, Tome W. SUET650: Evaluation of novel IMRT autoplanning tool for nasopharyngeal carcinoma cases. Med Phys 2013;40:355. 
20.  Hazell I, Bzdusek K, Kumar P, Hansen CR, Bertelsen A, Eriksen JG, et al. Automatic planning of head and neck treatment plans. J Appl Clin Med Phys 2016;17:5901. 
[Figure 1], [Figure 2], [Figure 3]
[Table 1], [Table 2], [Table 3]
