In nearly homogeneous water, many commercial algorithms appear more similar than they really are. The difference appears when the beam crosses the lung, re-enters an air cavity, passes through dense bone or touches metal. This is where simplified physics starts to take its toll.<\/p>\n
Therefore, the comparison that matters is not \u201cwhich TPS seems more sophisticated\u201d, but what happens when the dose needs to cross:<\/p>\n
This article organizes the problem by clinical scenario. The useful question is not who wins an abstract contest between Pencil Beam<\/span>, AAA<\/span>, collapsed cone<\/span>, Acuros XB<\/span> and Monte Carlo<\/span>. The useful question is another: which hypothesis of each family begins to break when the medium stops looking like almost homogeneous water.<\/p>\n The lung remains one of the best stresses for any dose engine. Low density alters the transport of charged particles, increases penumbra, changes electronic balance and makes reentry into soft tissue especially sensitive to the model used.<\/p>\n Classical Pencil Beam<\/span> suffers here because its strength lies in corrections along the beam’s main axis, not in robust lateral treatment of heterogeneity. In lung terms, this difference takes a quick toll:<\/p>\n The underlying problem is that the algorithm tries to solve a strongly three-dimensional phenomenon with simplified lateral physics.<\/p>\n Classical AAA<\/span> greatly improves the picture because it incorporates:<\/p>\n But the Varian manual itself admits clear lung limitations. For 4\u20136 MV<\/span> and fields \u2265 5×5 cm\u00b2<\/span>, the algorithm tends to underestimate dose in the lung and overestimate dose in tissue equivalent to water after the lung. At higher energies (10\u201320 MV<\/span>) and fields \u2264 5×5 cm\u00b2<\/span>, it tends to overestimate the lung dose, with the error increasing as the field and lung density decrease.<\/p>\n The text of the Handbook of Radiotherapy Physics<\/span> reinforces this reading by commenting on benchmarks in which AAA<\/span> overestimated the pulmonary dose in small, high-energy beams.<\/p>\n collapsed cone<\/span> methods were exactly an answer to part of this problem. The handbook highlights that implementations of the CCC family<\/span> can, with good precision, represent:<\/p>\n This already puts CCC family<\/span> at a physically stronger level than the more classic Pencil Beam<\/span> at low density.<\/p>\n In lung, this is where the difference in algorithmic family becomes clearer. The handbook cites comparisons between EGSnrc<\/span>, Acuros XB<\/span> and AAA<\/span> in phantom with low density heterogeneity, showing good agreement between Acuros XB<\/span> and EGSnrc<\/span> in an extreme situation, while AAA<\/span> fails to adequately reproduce the dose within and below the heterogeneity.<\/p>\n In other words: lung is a scenario in which engines based on explicit transport or Monte Carlo<\/span> usually show their gain more clearly.<\/p>\n Air cavities, paranasal sinuses, airways and other air-tissue interfaces expose the limitation of algorithms that treat heterogeneity mainly as longitudinal correction.<\/p>\n Air-to-fabric interfaces challenge Pencil Beam<\/span> because of loss and recovery of electronic balance. When the algorithm does not represent the lateral transport of secondary particles with good fidelity, the dose at the interface and immediately after it tends to be less reliable.<\/p>\n Classical AAA<\/span> improves significantly compared to Pencil Beam<\/span> because it already handles multiple lateral directions via anisotropic kernels. But it still remains in the family of scaled kernels. This means that the interface description remains mediated by an approximation, not by explicit transport.<\/p>\n Air-fabric interfaces are one of the scenarios in which the formulation of the Acuros XB<\/span> and Monte Carlo<\/span> stops being a theoretical advantage and becomes a practical advantage. When the clinical question depends on how the dose reorganizes locally after passing through the air, the explicit transport solution tends to be more convincing.<\/p>\n A common mistake when comparing algorithms in heterogeneous media is to look only at an aggregate number, such as maximum dose, average or even a simplified coverage reading. Many of the most relevant differences appear in another form:<\/p>\n This is particularly important in lung and air cavities. Two algorithms may appear \u201csimilar\u201d in global metrics and yet disagree exactly in the region where clinical risk is concentrated.<\/p>\n If the lung is the classic test of low density, the bone is the classic test of the materiality of the problem. Here, it is no longer enough to treat the voxel as water with different density. The composition of the material begins to matter more visibly.<\/p>\n Algorithms that treat the medium primarily by water-equivalent scaling tend to capture part of the effect, but not all of the material difference.<\/p>\n In Acuros XB<\/span>, the CT to material mapping<\/span> and mass density place the bone on another level of physical description. This is why, in the dose to medium<\/span> versus dose to water<\/span>debate, bone repeatedly appears as the biological material in which the difference is no longer small.<\/p>\n Himself RayStation<\/span> warns that, when comparing different engines, the discrepancy between dose conventions can be relatively large in bone, on the order of 10%<\/span>. This data is important because it shows that part of the divergence between bone algorithms does not only come from the transport itself, but also from the way of reporting the dose.<\/p>\n Implants, prostheses and very dense materials put pressure on the dose calculation on several fronts:<\/p>\n Here, material-explicit algorithms gain importance, but they also require more discipline. The Varian manual highlights that Acuros XB<\/span> may block the calculation or require user intervention when densities exceed the range covered by automatic material assignment.<\/p>\n This detail shows an important clinical truth: in high Z<\/span>materials, more physical algorithms do not forgive poor case preparation. They are more powerful, but also more dependent on correct material representation.<\/p>\n In metal and high Z<\/span>, it is worth adding an important operational point: sometimes what appears to be a difference between algorithms is, in fact, a difference between the way each engine reacts to the same problematic image.<\/p>\n Artifact of CT<\/span>, inadequate calibration curve and lack of override<\/span> material can:<\/p>\n This is especially relevant when comparing material-explicit engines with more water-equivalent engines. Without properly treated imaging, the theoretical superiority of the more physical method may not appear cleanly.<\/p>\n Small field is a short word for a long physical problem. When the field decreases, penumbra occupies a larger fraction of the distribution, the electronic balance becomes more fragile and any simplification in lateral modeling or in the head weighs more.<\/p>\n It is the family that suffers most, especially in heterogeneity.<\/p>\n It can remain very competent in various contexts, but the Eclipse<\/span> manual highlights that relevant differences in the lung become more serious precisely when the fields are small and the energies high.<\/p>\n Classical IFU<\/span> local draws attention to another very important point: in small field rotational plans<\/span>, the calculation of RayStation<\/span> becomes highly sensitive to the parameters of MLC<\/span> of beam model. This is valuable because it prevents a frequent error. Not every difference in a small field is \u201cthe fault of the dose motor\u201d; some of it may come from the beam model and the MLC<\/span>.<\/p>\n Motors Monte Carlo<\/span> or closer to explicit transport often gain traction here, but this does not eliminate the importance of beam model, statistics, grid resolution and commissioning.<\/p>\n This table needs to be read maturely. It does not say that an algorithm \u201calways loses\u201d. It tells where each family’s dominant hypothesis tends to come under the most pressure.<\/p>\n There is a reading error that appears all the time in clinical comparisons: attributing every discrepancy to the name of the engine.<\/p>\n In heterogeneity, the observed difference can arise from several sources at the same time:<\/p>\n Himself RayStation<\/span> insists on this by saying that certain techniques, such as VMAT sequencing<\/span>, should be treated as practically a new technique, requiring validation of beam model and QA per patient. This completely changes the tone of the discussion. The dose algorithm matters a lot, but it never acts alone.<\/p>\n A more mature reading of the comparison between algorithms in heterogeneity includes at least four questions:<\/p>\n Without these questions, the comparison becomes a ranking. With them, it becomes clinical physics.<\/p>\n There is a final point worth highlighting: heterogeneity rarely appears alone in modern practice. It appears together with:<\/p>\n When this happens, the problem stops being just \u201chow the algorithm treats density\u201d and becomes \u201chow the algorithm + beam model + technique set describes a complex beam in a complex medium\u201d. This is exactly why regulatory texts like RayStation<\/span> insist so much on technique-specific validation and patient QA.<\/p>\n It is precisely in heterogeneity that names lose usefulness and physical hypotheses appear. Pencil Beam<\/span>, AAA<\/span>, collapsed cone<\/span>, Acuros XB<\/span> and Monte Carlo<\/span> do not disagree because \u201cis better\u201d in the abstract. They differ because they simplify different parts of the same problem.<\/p>\n In the lung and air-tissue interfaces, the laterality of transport becomes the protagonist. In bone and high Z<\/span>, the problem stops being just density and becomes material. In a small field, beam model, MLC<\/span> and discretization start to matter as much as the engine name.<\/p>\n If the team reads heterogeneity this way, the comparison between algorithms becomes much more useful. It stops being a branded debate and becomes a concrete question about where that calculation still holds and where it is already outside the comfortable zone.<\/p>\n","protected":false},"excerpt":{"rendered":" The most useful way to compare commercial algorithms is to see what each one does when the beam meets difficult materials.<\/p>\n","protected":false},"author":0,"featured_media":16998,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"om_disable_all_campaigns":false,"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"ngg_post_thumbnail":0,"fifu_image_url":"","fifu_image_alt":"","footnotes":""},"categories":[98,60],"tags":[],"class_list":{"0":"post-17211","1":"post","2":"type-post","3":"status-publish","4":"format-standard","5":"has-post-thumbnail","7":"category-radioterapia","8":"category-software"},"aioseo_notices":[],"rt_seo":{"title":"Commercial Algorithms in Heterogeneity: Lung, Bone, Air, ...","description":"Compare how Pencil Beam, AAA, collapsed cone, Acuros XB, and Monte Carlo behave in lung, bone, air, metal, and small fields.","canonical":"https:\/\/rtmedical.com.br\/dose-algorithms-heterogeneity-lung-bone-metal\/","og_image":"https:\/\/rtmedical.com.br\/wp-content\/uploads\/2026\/04\/kernel-deposicao-energia-monte-carlo.jpg","robots":"index,follow","schema_type":"Article","include_in_llms":true,"llms_label":"Guia t\u00e9cnico","llms_summary":"The most useful way to compare commercial algorithms is to see what each one does when the beam meets difficult materials.","faq_items":[],"video":[],"gtin":"","mpn":"","brand":"","aggregate_rating":[]},"_links":{"self":[{"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/posts\/17211\/"}],"collection":[{"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/posts\/"}],"about":[{"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/types\/post\/"}],"replies":[{"embeddable":true,"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/comments\/?post=17211"}],"version-history":[{"count":3,"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/posts\/17211\/revisions\/"}],"predecessor-version":[{"id":17274,"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/posts\/17211\/revisions\/17274\/"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/media\/16998\/"}],"wp:attachment":[{"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/media\/?parent=17211"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/categories\/?post=17211"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/rtmedical.com.br\/en\/wp-json\/wp\/v2\/tags\/?post=17211"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}In this Article<\/h2>\n
\n
Lung: the great test of algorithms’ honesty<\/h2>\n
Pencil Beam<\/h3>\n
\n
AAA<\/h3>\n
\n
Collapsed cone<\/h3>\n
\n
Acuros XB and Monte Carlo<\/h3>\n
Air-tissue interfaces: where lateral physics weighs heavily<\/h2>\n
What Pencil Beam tends to do badly<\/h3>\n
Where AAA improves and where it still suffers<\/h3>\n
Where Acuros and MC gain ground<\/h3>\n
Heterogeneity is not just a difference in maximum dose<\/h2>\n
\n
Bone: where the discussion stops being just heterogeneity and becomes material<\/h2>\n
What this means for older algorithms<\/h3>\n
What does this mean for Acuros XB<\/h3>\n
What does this mean for RayStation<\/h3>\n
Metal and high-Z materials: when the problem becomes even less \u201cwater-like\u201d<\/h2>\n
\n
Poor imaging can mask or amplify algorithmic differences<\/h2>\n
\n
Small fields: when simplification takes its toll<\/h2>\n
Pencil Beam<\/h3>\n
AAA<\/h3>\n
RayStation CC<\/h3>\n
MC and more physical engines<\/h3>\n
What each family tends to see best<\/h2>\n
\n\n
\n \nScenario<\/th>\n Families that tend to suffer most<\/th>\n Families that tend to respond best<\/th>\n<\/tr>\n<\/thead>\n \n Low density lung<\/td>\n Pencil Beam classic<\/td>\n Collapsed cone, Acuros XB, Monte Carlo<\/td>\n<\/tr>\n \n Soft tissue reentry after lung<\/td>\n Pencil Beam, AAA in certain scenarios<\/td>\n Acuros XB, Monte Carlo<\/td>\n<\/tr>\n \n Bone and dense interfaces<\/td>\n Strongly water-equivalent models<\/td>\n Acuros XB, Monte Carlo<\/td>\n<\/tr>\n \n Metal and high Z<\/td>\n Any algorithm without reliable material mapping<\/td>\n Well-configured material-explicit engines<\/td>\n<\/tr>\n \n Small heterogeneous fields<\/td>\n Pencil Beam, part of the simplified models<\/td>\n More physical engines, as long as they are well modeled<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n The classic error: blaming the algorithm when the problem is something else<\/h2>\n
\n
How to read heterogeneity more maturely<\/h2>\n
\n
What changes when heterogeneity meets modulation<\/h2>\n
\n