<figure><img src="image_477.png" /><figcaption>**Fig. 474.** Reheating consistent slow-roll predictions for N-Formalism Inflation 2 with $a = -0.2$ and $b = 3.5$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\tilde{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\tilde{x}_{\text{end}} \equiv (x_{\text{end}} - x_{\text{end}}^{\text{min}})/(x_{\text{end}}^{\text{max}} - x_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_478.png" /><figcaption>**Fig. 475.** Reheating consistent slow-roll predictions for N-Formalism Inflation 2 with $a = -0.01$ and $b = 3.5$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\hat{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\hat{x}_{\text{end}} \equiv (x_{\text{end}} - x_{\text{end}}^{\text{min}})/(x_{\text{end}}^{\text{max}} - x_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
A.93. N-Formalism Inflation 3 (NFI3)

See Figs. 476–481.

<figure><img src="image_479.png" /><figcaption>**Fig. 476.** Reheating consistent slow-roll predictions for N-Formalism Inflation 3 with $b = 0.05$ (inflation gracefully ends). Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the parameter $a < 0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll). See also Figs. 477 to 481 for other values of $b$.</figcaption></figure>
<figure><img src="image_480.png" /><figcaption>**Fig. 477.** Reheating consistent slow-roll predictions for N-Formalism Inflation 3 with $b = 0.25$ (inflation gracefully ends). Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the parameter $a < 0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_481.png" /><figcaption>**Fig. 478.** Reheating consistent slow-roll predictions for N-Formalism Inflation 3 with $b = 0.3$ (inflation gracefully ends). Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the parameter $a < 0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_482.png" /><figcaption>**Fig. 479.** Reheating consistent slow-roll predictions for N-Formalism Inflation 3 with $b = -0.1$ (inflation gracefully ends). Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the parameter $a > 0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_483.png" /><figcaption>**Fig. 480.** Reheating consistent slow-roll predictions for N-Formalism Inflation 3 with $b = -1.1$ (inflation gracefully ends). Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the parameter $a > 0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_484.png" /><figcaption>**Fig. 481.** Reheating consistent slow-roll predictions for N-Formalism Inflation 3 with $b = -2.1$ (inflation gracefully ends). Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the parameter $a > 0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
A.94. N-Formalism Inflation 4 (NFI4)

See Figs. 482–487.

<figure><img src="image_485.png" /><figcaption>**Fig. 482.** Reheating consistent slow-roll predictions for N-Formalism Inflation 4 with $a = 0.1$ and $b = 0.6$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\tilde{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\tilde{x}_{\text{end}} \equiv (x_{\text{end}} - x_{\text{end}}^{\text{min}})/(x_{\text{end}}^{\text{max}} - x_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll). See also Figs. 483 to 487 for other values of $a$ and $b$.</figcaption></figure>
<figure><img src="image_486.png" /><figcaption>**Fig. 483.** Reheating consistent slow-roll predictions for N-Formalism Inflation 4 with $a = 0.2$ and $b = 0.6$. Predictions are represented in the plane $(n_c, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\hat{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\hat{x}_{\text{end}} \equiv (x_{\text{end}} - x_{\text{end}}^{\text{min}})/(x_{\text{end}}^{\text{max}} - x_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_487.png" /><figcaption>**Fig. 484.** Reheating consistent slow-roll predictions for N-Formalism Inflation 4 with $a = 0.1$ and $b = 0.8$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\hat{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\hat{x}_{\text{end}} \equiv (x_{\text{end}} - x_{\text{end}}^{\text{min}})/(x_{\text{end}}^{\text{max}} - x_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_488.png" /><figcaption>**Fig. 485.** Reheating consistent slow-roll predictions for N-Formalism Inflation 4 with $a = -1.0$ and $b = -1.5$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\tilde{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\tilde{x}_{\text{end}} \equiv (x_{\text{end}} - x_{\text{end}}^{\text{min}})/(x_{\text{end}}^{\text{max}} - x_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_489.png" /><figcaption>**Fig. 486.** Reheating consistent slow-roll predictions for N-Formalism Inflation 4 with $a = -0.1$ and $b = -1.5$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\tilde{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\tilde{x}_{\text{end}} \equiv (x_{\text{end}} - x_{\text{end}}^{\text{min}})/(x_{\text{end}}^{\text{max}} - x_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_490.png" /><figcaption>**Fig. 487.** Reheating consistent slow-roll predictions for N-Formalism Inflation 4 with $a = -1$ and $b = -5$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of the normalized field values $\hat{x}_{\text{end}}$ at which inflation ends. This one is varied within its maximal allowed range, i.e. with $\hat{x}_{\text{end}} \equiv (x_{\text{end}} - \chi_{\text{end}}^{\text{min}})/(\chi_{\text{end}}^{\text{max}} - \chi_{\text{end}}^{\text{min}})$ in the domain $[0, 1]$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
A.95. Radiatively Corrected Inflection Point Inflation 1 (RCIPI1)

See Figs. 488–502.

<figure><img src="image_491.png" /><figcaption>**Fig. 488.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 2$, $\beta = 1$ and when the potential has almost an inflection point. This one occurs for $\alpha = -\alpha_1$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha + \alpha_1$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll). See also Figs. 489 to 493 for other values of $p$ and $\beta$.</figcaption></figure>
<figure><img src="image_492.png" /><figcaption>**Fig. 489.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 2$, $\beta = 1.5$ and when the potential has almost an inflection point. This one occurs for $\alpha = -\alpha_0$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha + \alpha_0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_493.png" /><figcaption>**Fig. 490.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 2$, $\beta = 2$ and when the potential has almost an inflection point. This one occurs for $\alpha = -\alpha_0$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha + \alpha_0$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_494.png" /><figcaption>**Fig. 491.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 4$, $\beta = 7$ and when the potential has almost an inflection point. This one occurs for $\alpha = -\alpha_t$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha + \alpha_t$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_495.png" /><figcaption>**Fig. 492.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 4$, $\beta = 8$ and when the potential has almost an inflection point. This one occurs for $\alpha = -\alpha$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha + \alpha_i$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_496.png" /><figcaption>**Fig. 493.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 4$, $\beta = 9$ and when the potential has almost an inflection point. This one occurs for $\alpha = -\alpha_t$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha + \alpha_t$. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_497.png" /><figcaption>**Fig. 494.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 2$ and $\beta = 0.06$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\tilde{a} \equiv (2\sqrt{\tilde{\beta}} + \alpha)/(2\sqrt{\tilde{\beta}} - \alpha)$. This one is varied within its maximal allowed range [0, 1] for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll). See also Figs. 495 to 502 for other values of $p$ and $\beta$.</figcaption></figure>
<figure><img src="image_498.png" /><figcaption>**Fig. 495.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 2$ and $\dot{\beta} = 0.08$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(c_1, c_2)$ (bottom panel) for various values of $\dot{a} \equiv (2\sqrt{\dot{\beta}} + \alpha)/(2\sqrt{\dot{\beta}} - \alpha_c)$. This one is varied within its maximal allowed range [0, 1] for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_499.png" /><figcaption>**Fig. 496.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 2$ and $\beta = 0.1$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (2\sqrt{\bar{\beta}} + \alpha)/(2\sqrt{\bar{\beta}} - \alpha_n)$. This one is varied within its maximal allowed range [0, 1] for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_500.png" /><figcaption>**Fig. 497.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 3$ and $\beta = 0.06$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (2\sqrt{\hat{\beta}} + \alpha)/(2\sqrt{\hat{\beta}} - \alpha_c)$. This one is varied within its maximal allowed range $[0, 1]$ for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_501.png" /><figcaption>**Fig. 498.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 3$ and $\beta = 0.08$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(c_1, c_2)$ (bottom panel) for various values of $\dot{a} \equiv (2\sqrt{\bar{\beta}} + \alpha)/(2\sqrt{\bar{\beta}} - \alpha_c)$. This one is varied within its maximal allowed range [0, 1] for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_502.png" /><figcaption>**Fig. 499.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 3$ and $\beta = 0.1$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (2\sqrt{\bar{\beta}} + \alpha)/(2\sqrt{\bar{\beta}} - \alpha_n)$. This one is varied within its maximal allowed range [0, 1] for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_503.png" /><figcaption>**Fig. 500.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 4$ and $\beta = 0.06$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (2\sqrt{\hat{\beta}} + \alpha)/(2\sqrt{\hat{\beta}} - \alpha_c)$. This one is varied within its maximal allowed range $[0, 1]$ for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_504.png" /><figcaption>**Fig. 501.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 4$ and $\beta = 0.08$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(c_1, c_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (2\sqrt{\hat{\beta}} + \alpha)/(2\sqrt{\hat{\beta}} - \alpha_c)$. This one is varied within its maximal allowed range $[0, 1]$ for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_505.png" /><figcaption>**Fig. 502.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 1 for $p = 4$ and $\beta = 0.1$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (2\sqrt{\tilde{\beta}} + \alpha)/(2\sqrt{\tilde{\beta}} - \alpha_n)$. This one is varied within its maximal allowed range [0, 1] for triggering the RCIPI1 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
A.96. Radiatively Corrected Inflection Point Inflation 2 (RCIPI2)

See Figs. 503–513.

<figure><img src="image_506.png" /><figcaption>Fig. 503. Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 2$, $\beta = 2$ and when the potential is monotonic. The limiting case of an inflection point occurs for $\alpha = \pm 2$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha$ ranging within the maximal domain $|r| - 2.2|\epsilon_2|$ supporting RCIPI2. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll). See also Fig. 504.</figcaption></figure>
<figure><img src="image_507.png" /><figcaption>**Fig. 504.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 4$, $\beta = 8$ and when the potential is monotonic. The limiting case of an inflection point occurs for $\alpha = \pm 4$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\alpha$ ranging within the whole domain $]-4, 4[$ supporting RCIPI2. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_508.png" /><figcaption>**Fig. 505.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 2$ and $\beta = 0.05$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(c_1, c_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (\alpha + \alpha_p)/(2\alpha_o)$. This one is varied within its maximal allowed range $]0, 1[$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll). See also Figs. 491 to 498 for other values of $p$ and $\beta$.</figcaption></figure>
<figure><img src="image_509.png" /><figcaption>**Fig. 506.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 2$ and $\beta = 0.1$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (\alpha + \alpha_0)/(2\alpha_0)$. This one is varied within its maximal allowed range $|\alpha|, 1$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_510.png" /><figcaption>Fig. 507. Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 2$ and $\beta = 0.15$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(c_1, c_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (\alpha + \alpha_0)/(2\alpha_0)$. This one is varied within its maximal allowed range $[0, 1[$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_511.png" /><figcaption>**Fig. 508.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 3$ and $\beta = 0.05$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\dot{\alpha} \equiv (\alpha + \alpha_*)/(2\alpha_*)$. This one is varied within its maximal allowed range $|0, 1|$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_512.png" /><figcaption>**Fig. 509.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 3$ and $\beta = 0.1$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (\alpha + \alpha_*)/(2\alpha_*)$. This one is varied within its maximal allowed range $|0, 1|$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_513.png" /><figcaption>**Fig. 510.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 3$ and $\beta = 0.15$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\dot{\alpha} \equiv (\alpha + \alpha_*)/(2\alpha_*)$. This one is varied within its maximal allowed range $|0, 1|$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_514.png" /><figcaption>**Fig. 511.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 4$ and $\beta = 0.05$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\dot{\alpha} \equiv (\alpha + \alpha_*)/(2\alpha_*)$. This one is varied within its maximal allowed range $|0, 1|$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_515.png" /><figcaption>**Fig. 512.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 4$ and $\beta = 0.1$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(\epsilon_1, \epsilon_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (\alpha + \alpha_0)/(2\alpha_0)$. This one is varied within its maximal allowed range $|\alpha|, 1$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
<figure><img src="image_516.png" /><figcaption>**Fig. 513.** Reheating consistent slow-roll predictions for Radiatively Corrected Inflection Point Inflation 2 for $p = 4$ and $\beta = 0.15$. Predictions are represented in the plane $(n_s, r)$ (top panel) and in the plane $(c_1, c_2)$ (bottom panel) for various values of $\hat{\alpha} \equiv (\alpha + \alpha_0)/(2\alpha_0)$. This one is varied within its maximal allowed range $|0, 1|$ for triggering the RCIPI2 regime. The solid contours are the one and two-sigma Planck 2018 + Bicep-Keck confidence intervals (marginalized over second order slow-roll).</figcaption></figure>
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