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style-src 'unsafe-inline'; base-uri 'none'; img-src data:\" http-equiv=\"Content-Security-Policy\"/><title>SOL 1W ATM eases as downside skew deepens</title><style>:root { color-scheme: light; --paper: #f7f3eb; --raised: #f0ebe1; --ink: #242824; --soft: #3d433e; --muted: #626a61; --line: #d3cec2; --strong: #b5b5a7; --teal: #315f59; --teal-pale: #e3ebe3; }\n* { box-sizing: border-box; }\nhtml { background: var(--paper); }\nbody { margin: 0; background: var(--paper); color: var(--ink); font: 16px/1.6 system-ui, -apple-system, BlinkMacSystemFont, \"Segoe UI\", sans-serif; }\na { color: var(--teal); text-underline-offset: 3px; overflow-wrap: anywhere; }\na:focus-visible, summary:focus-visible { outline: 2px solid var(--teal); outline-offset: 4px; }\n.report { width: calc(100% - 48px); max-width: 1100px; width: min(calc(100% - 48px), 1100px); margin: 0 auto; padding-bottom: 56px; }\n.hero { padding: 24px 0 32px; border-bottom: 1px solid var(--strong); }\n.brand-row { display: flex; justify-content: space-between; 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}\n  .appendix { break-before: page; }\n  .appendix pre { max-height: none; overflow: visible; }\n  .appendix:not([open]) > *:not(summary), .chart-data:not([open]) > *:not(summary), .retrieval-details:not([open]) > *:not(summary) { display: none !important; }\n  a { color: inherit; }\n}\n\n.chart-scroll {max-width:100%; overflow-x:auto;} .chart-scroll svg {min-width:760px;} .series-key {display:inline-block; width:18px; height:3px; vertical-align:middle; margin-right:5px;} .figure-reference {font:12px system-ui,sans-serif;} .consolidated-limits {max-width:760px;}\n@media (max-width: 760px) { .research-panel table, .market-scorecard table { min-width: 740px; } .appendix { overflow-wrap: anywhere; } }</style><style>img.brand-mark {display:block; width:30px; height:30px; background:none;} .snapshot > div {padding-top:10px; padding-bottom:10px;} .snapshot strong {margin:2px 0;}</style></head><body><main class=\"report\"><header class=\"hero\"><div class=\"brand-row\"><img alt=\"\" aria-hidden=\"true\" class=\"brand-mark\" src=\"data:image/svg+xml;base64,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\"/> DERIVASYS</div><p class=\"eyebrow\">Focused research note</p><h1>SOL 1W ATM eases as downside skew deepens</h1><p class=\"standfirst\">SOL’s 1W at-the-money volatility declined while downside asymmetry deepened and the butterfly premium widened. The distinction matters: lower 1W ATM volatility accompanied greater relative pricing of downside protection and wings, while longer-tenor ATM volatility increased.</p><p class=\"byline\">Derivasys Research</p><div aria-label=\"Report snapshot\" class=\"snapshot\"><div><span>Report date</span><strong>06 Nov 2026</strong></div><div><span>Current snapshot</span><strong>06 Nov 2026 · 17:31 UTC</strong></div><div><span>Coverage</span><strong>SOL</strong></div><div><span>Comparison snapshot</span><strong>05 Nov 2026 · 17:31 UTC</strong></div></div></header><section class=\"section editorial\"><p class=\"eyebrow\">The reading</p><h2>What the evidence says</h2><p class=\"finding\">SOL’s 1W ATM, or at-the-money implied volatility, changed by -4.89 vol points <sup class=\"source-mark\"><a aria-label=\"Source 1\" href=\"#source-1\">[1]</a></sup> to 57.24% <sup class=\"source-mark\"><a aria-label=\"Source 2\" href=\"#source-2\">[2]</a></sup> over the crypto comparison window. This easing accompanied a deeper existing downside bias: 1W RR25, the call-versus-put IV asymmetry, moved from -0.19 vol points <sup class=\"source-mark\"><a aria-label=\"Source 3\" href=\"#source-3\">[3]</a></sup> to -4.22 vol points <sup class=\"source-mark\"><a aria-label=\"Source 4\" href=\"#source-4\">[4]</a></sup>, changing by -4.03 vol points <sup class=\"source-mark\"><a aria-label=\"Source 5\" href=\"#source-5\">[5]</a></sup>. Meanwhile, 1W BF25—the average wing IV premium over ATM—changed by +0.54 vol points <sup class=\"source-mark\"><a aria-label=\"Source 6\" href=\"#source-6\">[6]</a></sup> to 1.60 vol points <sup class=\"source-mark\"><a aria-label=\"Source 7\" href=\"#source-7\">[7]</a></sup>. The economic signal is a reshaping of the 1W smile: its center eased while downside asymmetry and the relative wing premium increased.</p><p class=\"finding\">The 1W ATM decline contrasts with increases further along SOL’s curve. Over the same crypto window, 1M ATM changed by +1.14 vol points <sup class=\"source-mark\"><a aria-label=\"Source 8\" href=\"#source-8\">[8]</a></sup> to 55.50% <sup class=\"source-mark\"><a aria-label=\"Source 9\" href=\"#source-9\">[9]</a></sup>; 2M ATM changed by +2.00 vol points <sup class=\"source-mark\"><a aria-label=\"Source 10\" href=\"#source-10\">[10]</a></sup>, and 3M ATM by +2.66 vol points <sup class=\"source-mark\"><a aria-label=\"Source 11\" href=\"#source-11\">[11]</a></sup>. Despite these opposing changes, 1W ATM remained above 1M ATM, preserving an inverted relationship between those tenors. Smile repricing also extended beyond 1W: 1M RR25 changed by -0.69 vol points <sup class=\"source-mark\"><a aria-label=\"Source 12\" href=\"#source-12\">[12]</a></sup> to -0.40 vol points <sup class=\"source-mark\"><a aria-label=\"Source 13\" href=\"#source-13\">[13]</a></sup>, crossing from positive to negative. The 1M BF25 premium changed by +0.36 vol points <sup class=\"source-mark\"><a aria-label=\"Source 14\" href=\"#source-14\">[14]</a></sup> to 1.83 vol points <sup class=\"source-mark\"><a aria-label=\"Source 15\" href=\"#source-15\">[15]</a></sup>, while 2W BF25 changed by +0.59 vol points <sup class=\"source-mark\"><a aria-label=\"Source 16\" href=\"#source-16\">[16]</a></sup> to 1.67 vol points <sup class=\"source-mark\"><a aria-label=\"Source 17\" href=\"#source-17\">[17]</a></sup>. The 2W butterfly adjustment therefore rules out describing the relative wing repricing as confined to 1W.</p><p class=\"finding\">The magnitude of SOL’s 1W BF25 adjustment stands out within its eligible rolling-window history. Its absolute daily move ranked at 100th percentile <sup class=\"source-mark\"><a aria-label=\"Source 18\" href=\"#source-18\">[18]</a></sup>, with sample size and bounds of 30 observations (observed sampling; 07 Oct 2026–05 Nov 2026) <sup class=\"source-mark\"><a aria-label=\"Source 18\" href=\"#source-18\">[18]</a></sup>. This comparison supports attention to the 1W butterfly premium specifically; it does not establish that the combined ATM, skew and butterfly configuration is historically unusual.</p><p class=\"finding\">Spot and realized volatility qualify the interpretation of SOL’s 1W options easing. SOL’s spot return over the crypto comparison window was +0.56% <sup class=\"source-mark\"><a aria-label=\"Source 19\" href=\"#source-19\">[19]</a></sup>, so the deepening negative 1W RR25 accompanied a positive spot return. Trailing realized volatility, recomputed from canonical minute log returns over the weekly window, was 59.38% <sup class=\"source-mark\"><a aria-label=\"Source 20\" href=\"#source-20\">[20]</a></sup>. Forward 1W ATM IV minus that trailing realized measure was -2.14 vol points <sup class=\"source-mark\"><a aria-label=\"Source 21\" href=\"#source-21\">[21]</a></sup>. This negative spread places the lower 1W ATM quote below the measured trailing realized level, but the different forward and backward periods prevent a forecast or a cheapness conclusion.</p><div class=\"consolidated-limits\"><h3>Qualifications and limits</h3><ul><li>BF25 measures a premium relative to ATM; its increase does not independently establish an increase in absolute average wing IV or directional demand.</li><li>Historical ranks describe eligible observed samples with their native daily horizons; selection and missing dates can affect the comparison. They are neither population rarity estimates nor joint significance tests.</li><li>The spot and options changes share the crypto comparison endpoints; trailing realized volatility covers an earlier weekly interval and uses a calendar-year annualization basis with complete observed minute-return coverage. These descriptive relationships do not identify a catalyst, investor positioning or a trading edge.</li></ul></div></section><section class=\"section market-scorecard\"><h2>Verified market snapshot</h2><div class=\"table-wrap\"><table><caption>Current levels and changes over each recorded native interval. Only receipt-matched quotes are shown; an em dash marks a missing matching quote.</caption><thead><tr><th scope=\"col\">Asset · tenor</th><th scope=\"col\">ATM IV</th><th scope=\"col\">ATM IV change</th><th scope=\"col\">RR25</th><th scope=\"col\">RR25 change</th><th scope=\"col\">BF25 change</th></tr></thead><tbody><tr><th scope=\"row\">SOL · 1W</th><td>57.24 %<sup class=\"source-mark\"><a aria-label=\"Source 2\" href=\"#source-2\">[2]</a></sup></td><td>-4.89 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 1\" href=\"#source-1\">[1]</a></sup></td><td>-4.22 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 4\" href=\"#source-4\">[4]</a></sup></td><td>-4.03 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 5\" href=\"#source-5\">[5]</a></sup></td><td>0.54 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 6\" href=\"#source-6\">[6]</a></sup></td></tr><tr><th scope=\"row\">SOL · 2W</th><td>56.70 %<sup class=\"source-mark\"><a aria-label=\"Source 22\" href=\"#source-22\">[22]</a></sup></td><td>1.06 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 23\" href=\"#source-23\">[23]</a></sup></td><td>-2.76 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 24\" href=\"#source-24\">[24]</a></sup></td><td>-3.32 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 25\" href=\"#source-25\">[25]</a></sup></td><td>0.59 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 16\" href=\"#source-16\">[16]</a></sup></td></tr><tr><th scope=\"row\">SOL · 1M</th><td>55.50 %<sup class=\"source-mark\"><a aria-label=\"Source 9\" href=\"#source-9\">[9]</a></sup></td><td>1.14 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 8\" href=\"#source-8\">[8]</a></sup></td><td>-0.40 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 13\" href=\"#source-13\">[13]</a></sup></td><td>-0.69 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 12\" href=\"#source-12\">[12]</a></sup></td><td>0.36 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 14\" href=\"#source-14\">[14]</a></sup></td></tr><tr><th scope=\"row\">SOL · 2M</th><td>55.34 %<sup class=\"source-mark\"><a aria-label=\"Source 26\" href=\"#source-26\">[26]</a></sup></td><td>2.00 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 10\" href=\"#source-10\">[10]</a></sup></td><td>0.37 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 27\" href=\"#source-27\">[27]</a></sup></td><td>-0.45 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 28\" href=\"#source-28\">[28]</a></sup></td><td>0.34 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 29\" href=\"#source-29\">[29]</a></sup></td></tr><tr><th scope=\"row\">SOL · 3M</th><td>55.39 %<sup class=\"source-mark\"><a aria-label=\"Source 30\" href=\"#source-30\">[30]</a></sup></td><td>2.66 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 11\" href=\"#source-11\">[11]</a></sup></td><td>0.65 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 31\" href=\"#source-31\">[31]</a></sup></td><td>-0.81 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 32\" href=\"#source-32\">[32]</a></sup></td><td>0.28 vol pts<sup class=\"source-mark\"><a aria-label=\"Source 33\" href=\"#source-33\">[33]</a></sup></td></tr></tbody></table></div></section><section class=\"section curve-regimes\"><h2>Weekly versus monthly curve</h2><div class=\"table-wrap\"><table><caption>Matched native endpoints; inverted means monthly ATM IV is below weekly ATM IV. Regimes compare verified levels; no numerical slope is inferred.</caption><thead><tr><th scope=\"col\">Asset</th><th scope=\"col\">Prior 1W</th><th scope=\"col\">Prior 1M</th><th scope=\"col\">Current 1W</th><th scope=\"col\">Current 1M</th><th scope=\"col\">Curve regime</th></tr></thead><tbody><tr><th scope=\"row\">SOL</th><td>62.13 % <sup class=\"source-mark\"><a aria-label=\"Source 34\" href=\"#source-34\">[34]</a></sup></td><td>54.36 % <sup class=\"source-mark\"><a aria-label=\"Source 35\" href=\"#source-35\">[35]</a></sup></td><td>57.24 % <sup class=\"source-mark\"><a aria-label=\"Source 2\" href=\"#source-2\">[2]</a></sup></td><td>55.50 % <sup class=\"source-mark\"><a aria-label=\"Source 9\" href=\"#source-9\">[9]</a></sup></td><td>Remained inverted</td></tr></tbody></table></div></section><section class=\"section chart-section thesis-figure\"><h2>SOL BF25 curve</h2><figure><div aria-label=\"Scrollable figure\" class=\"chart-scroll\" role=\"region\" tabindex=\"0\"><svg aria-label=\"SOL BF25 curve\" role=\"img\" viewbox=\"0 0 760 285\"><title>SOL BF25 curve</title><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"32.00\">2.05 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"84.50\">1.80 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"137.00\">1.55 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"189.50\">1.31 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"242.00\">1.06 vol pts</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"125.00\" y=\"265\">1W</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"273.75\" y=\"265\">2W</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"422.50\" y=\"265\">1M</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"571.25\" y=\"265\">2M</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"720.00\" y=\"265\">3M</text><circle cx=\"125.00\" cy=\"123.45\" fill=\"#315f59\" r=\"4\"><title>1W · Current · 06 Nov 2026 · 17:31 UTC: 1.60 vol pts</title></circle><path d=\"M125.00,123.45 L273.75,108.61\" fill=\"none\" stroke=\"#315f59\" stroke-width=\"2\"></path><circle cx=\"273.75\" cy=\"108.61\" fill=\"#315f59\" r=\"4\"><title>2W · Current · 06 Nov 2026 · 17:31 UTC: 1.67 vol pts</title></circle><path d=\"M273.75,108.61 L422.50,74.67\" fill=\"none\" stroke=\"#315f59\" stroke-width=\"2\"></path><circle cx=\"422.50\" cy=\"74.67\" fill=\"#315f59\" r=\"4\"><title>1M · Current · 06 Nov 2026 · 17:31 UTC: 1.83 vol pts</title></circle><path d=\"M422.50,74.67 L571.25,28.00\" fill=\"none\" stroke=\"#315f59\" stroke-width=\"2\"></path><circle cx=\"571.25\" cy=\"28.00\" fill=\"#315f59\" r=\"4\"><title>2M · Current · 06 Nov 2026 · 17:31 UTC: 2.05 vol pts</title></circle><path d=\"M571.25,28.00 L720.00,34.36\" fill=\"none\" stroke=\"#315f59\" stroke-width=\"2\"></path><circle cx=\"720.00\" cy=\"34.36\" fill=\"#315f59\" r=\"4\"><title>3M · Current · 06 Nov 2026 · 17:31 UTC: 2.02 vol pts</title></circle><circle cx=\"125.00\" cy=\"238.00\" fill=\"#9a8260\" r=\"4\"><title>1W · Comparison · 05 Nov 2026 · 17:31 UTC: 1.06 vol pts</title></circle><path d=\"M125.00,238.00 L273.75,233.76\" fill=\"none\" stroke=\"#9a8260\" stroke-dasharray=\"7 5\" stroke-width=\"2\"></path><circle cx=\"273.75\" cy=\"233.76\" fill=\"#9a8260\" r=\"4\"><title>2W · Comparison · 05 Nov 2026 · 17:31 UTC: 1.08 vol pts</title></circle><path d=\"M273.75,233.76 L422.50,151.03\" fill=\"none\" stroke=\"#9a8260\" stroke-dasharray=\"7 5\" stroke-width=\"2\"></path><circle cx=\"422.50\" cy=\"151.03\" fill=\"#9a8260\" r=\"4\"><title>1M · Comparison · 05 Nov 2026 · 17:31 UTC: 1.47 vol pts</title></circle><path d=\"M422.50,151.03 L571.25,100.12\" fill=\"none\" stroke=\"#9a8260\" stroke-dasharray=\"7 5\" stroke-width=\"2\"></path><circle cx=\"571.25\" cy=\"100.12\" fill=\"#9a8260\" r=\"4\"><title>2M · Comparison · 05 Nov 2026 · 17:31 UTC: 1.71 vol pts</title></circle><path d=\"M571.25,100.12 L720.00,93.76\" fill=\"none\" stroke=\"#9a8260\" stroke-dasharray=\"7 5\" stroke-width=\"2\"></path><circle cx=\"720.00\" cy=\"93.76\" fill=\"#9a8260\" r=\"4\"><title>3M · Comparison · 05 Nov 2026 · 17:31 UTC: 1.74 vol pts</title></circle></svg></div><figcaption><span><i class=\"series-key\" style=\"background:#315f59\"></i>Current · 06 Nov 2026 · 17:31 UTC</span> · <span><i class=\"series-key\" style=\"background:#9a8260\"></i>Comparison · 05 Nov 2026 · 17:31 UTC</span>. Tenors are equally spaced categories, not elapsed time. Gaps remain unconnected.</figcaption></figure></section><p class=\"source-note\">Figure sources: <sup class=\"source-mark\"><a aria-label=\"Source 41\" href=\"#source-41\">[41]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 42\" href=\"#source-42\">[42]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 43\" href=\"#source-43\">[43]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 44\" href=\"#source-44\">[44]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 45\" href=\"#source-45\">[45]</a></sup></p><section class=\"section chart-section thesis-figure\"><h2>SOL: size of daily changes in the 1-week butterfly premium (BF25)</h2><figure><div aria-label=\"Scrollable figure\" class=\"chart-scroll\" role=\"region\" tabindex=\"0\"><svg aria-label=\"SOL: size of daily changes in the 1-week butterfly premium (BF25) ranked observed sample\" role=\"img\" viewbox=\"0 0 760 285\"><title>SOL: size of daily changes in the 1-week butterfly premium (BF25)</title><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"32.00\">0.54 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"84.50\">0.41 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"137.00\">0.28 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"189.50\">0.14 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"242.00\">0.01 vol pts</text><circle cx=\"125.00\" cy=\"238.00\" fill=\"#315f59\" r=\"3\"><title>2026-10-21T17:31:00+00:00: 0.01 vol pts</title></circle><circle cx=\"145.52\" cy=\"238.00\" fill=\"#315f59\" r=\"3\"><title>2026-11-04T17:31:00+00:00: 0.01 vol pts</title></circle><circle cx=\"166.03\" cy=\"230.08\" fill=\"#315f59\" r=\"3\"><title>2026-10-30T17:31:00+00:00: 0.03 vol pts</title></circle><circle cx=\"186.55\" cy=\"218.19\" fill=\"#315f59\" r=\"3\"><title>2026-10-14T17:31:00+00:00: 0.06 vol pts</title></circle><circle cx=\"207.07\" cy=\"218.19\" fill=\"#315f59\" r=\"3\"><title>2026-10-27T17:31:00+00:00: 0.06 vol pts</title></circle><circle cx=\"227.59\" cy=\"218.19\" fill=\"#315f59\" r=\"3\"><title>2026-11-02T17:31:00+00:00: 0.06 vol pts</title></circle><circle cx=\"248.10\" cy=\"210.26\" fill=\"#315f59\" r=\"3\"><title>2026-10-11T17:31:00+00:00: 0.08 vol pts</title></circle><circle cx=\"268.62\" cy=\"210.26\" fill=\"#315f59\" r=\"3\"><title>2026-10-19T17:31:00+00:00: 0.08 vol pts</title></circle><circle cx=\"289.14\" cy=\"206.30\" fill=\"#315f59\" r=\"3\"><title>2026-10-17T17:31:00+00:00: 0.09 vol pts</title></circle><circle cx=\"309.66\" cy=\"198.38\" fill=\"#315f59\" r=\"3\"><title>2026-10-28T17:31:00+00:00: 0.11 vol pts</title></circle><circle cx=\"330.17\" cy=\"194.42\" fill=\"#315f59\" r=\"3\"><title>2026-10-25T17:31:00+00:00: 0.12 vol pts</title></circle><circle cx=\"350.69\" cy=\"186.49\" fill=\"#315f59\" r=\"3\"><title>2026-10-10T17:31:00+00:00: 0.14 vol pts</title></circle><circle cx=\"371.21\" cy=\"178.57\" fill=\"#315f59\" r=\"3\"><title>2026-10-26T17:31:00+00:00: 0.16 vol pts</title></circle><circle cx=\"391.72\" cy=\"178.57\" fill=\"#315f59\" r=\"3\"><title>2026-11-01T17:31:00+00:00: 0.16 vol pts</title></circle><circle cx=\"412.24\" cy=\"170.64\" fill=\"#315f59\" r=\"3\"><title>2026-10-15T17:31:00+00:00: 0.18 vol pts</title></circle><circle cx=\"432.76\" cy=\"170.64\" fill=\"#315f59\" r=\"3\"><title>2026-11-03T17:31:00+00:00: 0.18 vol pts</title></circle><circle cx=\"453.28\" cy=\"166.68\" fill=\"#315f59\" r=\"3\"><title>2026-10-18T17:31:00+00:00: 0.19 vol pts</title></circle><circle cx=\"473.79\" cy=\"166.68\" fill=\"#315f59\" r=\"3\"><title>2026-10-20T17:31:00+00:00: 0.19 vol pts</title></circle><circle cx=\"494.31\" cy=\"150.83\" fill=\"#315f59\" r=\"3\"><title>2026-10-09T17:31:00+00:00: 0.23 vol pts</title></circle><circle cx=\"514.83\" cy=\"150.83\" fill=\"#315f59\" r=\"3\"><title>2026-10-22T17:31:00+00:00: 0.23 vol pts</title></circle><circle cx=\"535.34\" cy=\"134.98\" fill=\"#315f59\" r=\"3\"><title>2026-10-23T17:31:00+00:00: 0.27 vol pts</title></circle><circle cx=\"555.86\" cy=\"134.98\" fill=\"#315f59\" r=\"3\"><title>2026-10-29T17:31:00+00:00: 0.27 vol pts</title></circle><circle cx=\"576.38\" cy=\"131.02\" fill=\"#315f59\" r=\"3\"><title>2026-10-12T17:31:00+00:00: 0.28 vol pts</title></circle><circle cx=\"596.90\" cy=\"127.06\" fill=\"#315f59\" r=\"3\"><title>2026-10-08T17:31:00+00:00: 0.29 vol pts</title></circle><circle cx=\"617.41\" cy=\"127.06\" fill=\"#315f59\" r=\"3\"><title>2026-10-16T17:31:00+00:00: 0.29 vol pts</title></circle><circle cx=\"637.93\" cy=\"123.09\" fill=\"#315f59\" r=\"3\"><title>2026-10-13T17:31:00+00:00: 0.30 vol pts</title></circle><circle cx=\"658.45\" cy=\"119.13\" fill=\"#315f59\" r=\"3\"><title>2026-11-05T17:31:00+00:00: 0.31 vol pts</title></circle><circle cx=\"678.97\" cy=\"99.32\" fill=\"#315f59\" r=\"3\"><title>2026-10-24T17:31:00+00:00: 0.36 vol pts</title></circle><circle cx=\"699.48\" cy=\"83.47\" fill=\"#315f59\" r=\"3\"><title>2026-10-07T17:31:00+00:00: 0.40 vol pts</title></circle><circle cx=\"720.00\" cy=\"71.58\" fill=\"#315f59\" r=\"3\"><title>2026-10-31T17:31:00+00:00: 0.43 vol pts</title></circle><circle class=\"current-statistic\" cx=\"720.00\" cy=\"28.00\" fill=\"#ac6353\" r=\"6\"><title>Current statistic: 0.54 vol pts</title></circle><text class=\"axis-label\" text-anchor=\"middle\" x=\"422.5\" y=\"265\">Sample rank (ordered by value)</text></svg></div><figcaption>Observed samples in teal. Current statistic: 0.54 vol pts (red). Change sizes ignore direction: increases and decreases of the same size are ranked together. BF25 is the average implied volatility of the 25-delta call and put minus at-the-money implied volatility. n=30; 2026-10-07 to 2026-11-05; source-selected observed sample, no fill.</figcaption></figure></section><p><sup class=\"source-mark\"><a aria-label=\"Source 18\" href=\"#source-18\">[18]</a></sup></p><section class=\"section chart-section thesis-figure\"><h2>BF25 change by tenor</h2><figure><div aria-label=\"Scrollable figure\" class=\"chart-scroll\" role=\"region\" tabindex=\"0\"><svg aria-label=\"BF25 change by tenor\" role=\"img\" viewbox=\"0 0 760 285\"><title>BF25 change by tenor</title><line stroke=\"#333\" x1=\"125\" x2=\"720\" y1=\"133.0\" y2=\"133.0\"></line><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"242.00\">-0.60 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"137.00\">0.00 vol pts</text><text class=\"axis-label\" text-anchor=\"end\" x=\"117\" y=\"32.00\">0.60 vol pts</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"224.17\" y=\"265\">1W</text><rect fill=\"#315f59\" height=\"94.50\" width=\"48.00\" x=\"200.17\" y=\"38.50\"><title>1W · SOL · 05 Nov 2026 · 17:31 UTC → 06 Nov 2026 · 17:31 UTC · 24h: 0.54 vol pts</title></rect><text class=\"axis-label\" text-anchor=\"middle\" x=\"224.17\" y=\"34.50\">0.54</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"422.50\" y=\"265\">2W</text><rect fill=\"#315f59\" height=\"103.25\" width=\"48.00\" x=\"398.50\" y=\"29.75\"><title>2W · SOL · 05 Nov 2026 · 17:31 UTC → 06 Nov 2026 · 17:31 UTC · 24h: 0.59 vol pts</title></rect><text class=\"axis-label\" text-anchor=\"middle\" x=\"422.50\" y=\"25.75\">0.59</text><text class=\"axis-label\" text-anchor=\"middle\" x=\"620.83\" y=\"265\">1M</text><rect fill=\"#315f59\" height=\"63.00\" width=\"48.00\" x=\"596.83\" y=\"70.00\"><title>1M · SOL · 05 Nov 2026 · 17:31 UTC → 06 Nov 2026 · 17:31 UTC · 24h: 0.36 vol pts</title></rect><text class=\"axis-label\" text-anchor=\"middle\" x=\"620.83\" y=\"66.00\">0.36</text></svg></div><figcaption><span><i class=\"series-key\" style=\"background:#315f59\"></i>SOL · 05 Nov 2026 · 17:31 UTC → 06 Nov 2026 · 17:31 UTC · 24h</span>. Own-run receipt-matched changes; missing or ambiguous points remain gaps.</figcaption></figure></section><p class=\"source-note\">Figure evidence: <sup class=\"source-mark\"><a aria-label=\"Source 6\" href=\"#source-6\">[6]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 16\" href=\"#source-16\">[16]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 14\" href=\"#source-14\">[14]</a></sup></p><section class=\"section research-panel\"><h2>What to watch next</h2><div class=\"table-wrap\"><table><caption>Each monitor describes a verified component or central counterexample of the selected story; observation tests, not a joint forecast.</caption><thead><tr><th scope=\"col\">Story component</th><th scope=\"col\">Next snapshot</th><th scope=\"col\">Observed condition</th><th scope=\"col\">Comparison period</th><th scope=\"col\">Evidence</th></tr></thead><tbody><tr><th scope=\"row\">SOL · 1W ATM implied volatility</th><td>07 Nov 2026 · 17:31 UTC</td><td>Current level: at or below 57.24 % (current level).<br/>Between current and prior: strictly above 57.24 % and strictly below 62.13 %.<br/>Prior level: at or above 62.13 % (prior level).</td><td>05 Nov 2026 · 17:31 UTC → 06 Nov 2026 · 17:31 UTC</td><td><sup class=\"source-mark\"><a aria-label=\"Source 2\" href=\"#source-2\">[2]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 34\" href=\"#source-34\">[34]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 1\" href=\"#source-1\">[1]</a></sup></td></tr><tr><th scope=\"row\">SOL · 1W 25-delta butterfly premium</th><td>07 Nov 2026 · 17:31 UTC</td><td>Current level: at or above 1.60 vol pts (current level).<br/>Between current and prior: strictly below 1.60 vol pts and strictly above 1.06 vol pts.<br/>Prior level: at or below 1.06 vol pts (prior level).</td><td>05 Nov 2026 · 17:31 UTC → 06 Nov 2026 · 17:31 UTC</td><td><sup class=\"source-mark\"><a aria-label=\"Source 7\" href=\"#source-7\">[7]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 46\" href=\"#source-46\">[46]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 6\" href=\"#source-6\">[6]</a></sup></td></tr><tr><th scope=\"row\">SOL · 1W 25-delta risk reversal</th><td>07 Nov 2026 · 17:31 UTC</td><td>Current level: at or below -4.22 vol pts (current level).<br/>Between current and prior: strictly above -4.22 vol pts and strictly below -0.19 vol pts.<br/>Prior level: at or above -0.19 vol pts (prior level).</td><td>05 Nov 2026 · 17:31 UTC → 06 Nov 2026 · 17:31 UTC</td><td><sup class=\"source-mark\"><a aria-label=\"Source 4\" href=\"#source-4\">[4]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 3\" href=\"#source-3\">[3]</a></sup> <sup class=\"source-mark\"><a aria-label=\"Source 5\" href=\"#source-5\">[5]</a></sup></td></tr></tbody></table></div></section><details class=\"appendix sampling-methodology\"><summary>Historical sampling methodology</summary><p>Each rank describes its supplied population. Exact consecutive daily endpoints use fixed UTC anchors and 24 elapsed hours, including across daylight-saving changes. Missing pairs are omitted without interpolation; their absence does not establish why the provider omitted them. Full captured history is bounded by this run. Different captures and windows can have different denominators even when their ranks agree.</p><div class=\"table-wrap\"><table><thead><tr><th>Measure</th><th>Population</th><th>Observed pairs or levels</th><th>Requested window</th><th>Excluded pair or level endpoints</th></tr></thead><tbody><tr><td>SOL 1W.bf25.absolute_move<sup class=\"source-mark\"><a aria-label=\"Source 18\" href=\"#source-18\">[18]</a></sup></td><td>rolling 30 calendar days (UTC)</td><td>30</td><td>2026-10-06T17:31:00+00:00 to 2026-11-05T17:31:00+00:00</td><td>None</td></tr></tbody></table></div></details><p class=\"clock-note bf-definition\">BF25 = (25-delta call IV + 25-delta put IV) / 2 − ATM IV. Levels and changes are measured in volatility points.</p><p>Retrospective report: native market dates are distinct from later retrieval and run clocks. Later capture does not establish availability at the original cutoff.</p><details class=\"section source-notes\"><summary>Source notes</summary><article id=\"source-1\"><h3>[1] SOL 1W ATM IV difference</h3><p>-4.89 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-2\"><h3>[2] SOL 1W ATM IV</h3><p>57.24 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-3\"><h3>[3] SOL 1W RR25</h3><p>-0.19 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-4\"><h3>[4] SOL 1W RR25</h3><p>-4.22 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-5\"><h3>[5] SOL 1W RR25 difference</h3><p>-4.03 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-6\"><h3>[6] SOL 1W BF25 difference</h3><p>0.54 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-7\"><h3>[7] SOL 1W BF25</h3><p>1.60 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-8\"><h3>[8] SOL 1M ATM IV difference</h3><p>1.14 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-9\"><h3>[9] SOL 1M ATM IV</h3><p>55.50 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-10\"><h3>[10] SOL 2M ATM IV difference</h3><p>2.00 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-11\"><h3>[11] SOL 3M ATM IV difference</h3><p>2.66 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-12\"><h3>[12] SOL 1M RR25 difference</h3><p>-0.69 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-13\"><h3>[13] SOL 1M RR25</h3><p>-0.40 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-14\"><h3>[14] SOL 1M BF25 difference</h3><p>0.36 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-15\"><h3>[15] SOL 1M BF25</h3><p>1.83 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-16\"><h3>[16] SOL 2W BF25 difference</h3><p>0.59 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-17\"><h3>[17] SOL 2W BF25</h3><p>1.67 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-18\"><h3>[18] SOL 1W BF25 absolute move percentile</h3><p>100.00 percentile</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-19\"><h3>[19] SOL spotPrice percentage change</h3><p>0.56 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-20\"><h3>[20] SOL rv7d.recomputed</h3><p>59.38 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-21\"><h3>[21] SOL 1W atmIv-rv7d spread</h3><p>-2.14 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-22\"><h3>[22] SOL 2W ATM IV</h3><p>56.70 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-23\"><h3>[23] SOL 2W ATM IV difference</h3><p>1.06 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-24\"><h3>[24] SOL 2W RR25</h3><p>-2.76 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-25\"><h3>[25] SOL 2W RR25 difference</h3><p>-3.32 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-26\"><h3>[26] SOL 2M ATM IV</h3><p>55.34 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-27\"><h3>[27] SOL 2M RR25</h3><p>0.37 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-28\"><h3>[28] SOL 2M RR25 difference</h3><p>-0.45 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-29\"><h3>[29] SOL 2M BF25 difference</h3><p>0.34 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-30\"><h3>[30] SOL 3M ATM IV</h3><p>55.39 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-31\"><h3>[31] SOL 3M RR25</h3><p>0.65 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-32\"><h3>[32] SOL 3M RR25 difference</h3><p>-0.81 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-33\"><h3>[33] SOL 3M BF25 difference</h3><p>0.28 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-34\"><h3>[34] SOL 1W ATM IV</h3><p>62.13 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-35\"><h3>[35] SOL 1M ATM IV</h3><p>54.36 %</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article><article id=\"source-41\"><h3>[41] Source</h3><p>Source type: options-observations</p><p>Observed: 2026-11-06T17:31:00+00:00</p><a href=\"https://api.derivasys.com/api/v1/history/snapshot\" rel=\"noopener noreferrer\" target=\"_blank\">Open cited source</a></article><article id=\"source-42\"><h3>[42] Source</h3><p>Source type: options-observations</p><p>Observed: 2026-11-06T17:31:00+00:00</p><a href=\"https://api.derivasys.com/api/v1/history/snapshot\" rel=\"noopener noreferrer\" target=\"_blank\">Open cited source</a></article><article id=\"source-43\"><h3>[43] Source</h3><p>Source type: options-observations</p><p>Observed: 2026-11-06T17:31:00+00:00</p><a href=\"https://api.derivasys.com/api/v1/history/snapshot\" rel=\"noopener noreferrer\" target=\"_blank\">Open cited source</a></article><article id=\"source-44\"><h3>[44] Source</h3><p>Source type: options-observations</p><p>Observed: 2026-11-06T17:31:00+00:00</p><a href=\"https://api.derivasys.com/api/v1/history/snapshot\" rel=\"noopener noreferrer\" target=\"_blank\">Open cited source</a></article><article id=\"source-45\"><h3>[45] Source</h3><p>Source type: options-observations</p><p>Observed: 2026-11-06T17:31:00+00:00</p><a href=\"https://api.derivasys.com/api/v1/history/snapshot\" rel=\"noopener noreferrer\" target=\"_blank\">Open cited source</a></article><article id=\"source-46\"><h3>[46] SOL 1W BF25</h3><p>1.06 vol pts</p><p>Source type: calculation</p><p>Observed: 2026-11-06T17:31:00+00:00</p></article></details></main></body></html>","provenance":{"canonicalReportSha256":"e5a850b4cedf2064add1f6ca7704622d447f84ca9564f0da125171cf57a6b0cd","presentationSha256":"2dc9080c27ab29789da106d9eb6e8600f1bca3b27229d1a7c3900b80cb2d1972","reviewedReportSha256":"e5a850b4cedf2064add1f6ca7704622d447f84ca9564f0da125171cf57a6b0cd","sourceHtmlSha256":"1afb6411c1ef41aa92677fe0e8c28595a0ac96beafa952283c4a87e8d6ab11b8","sourceJournalSha256":"7e9e48e8982364106d485bd50e1f976b49880782bfbe9e5513c51e6d45f5b7b0"},"reportDate":"2026-11-06","schemaVersion":1,"snapshotUtc":"2026-11-06T17:31:00+00:00","summary":"SOL’s 1W at-the-money volatility declined while downside asymmetry deepened and the butterfly premium widened. The distinction matters: lower 1W ATM volatility accompanied greater relative pricing of downside protection and wings, while longer-tenor ATM volatility increased.","title":"SOL 1W ATM eases as downside skew deepens"}