Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 2263 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{7}$ | 0.6835 | 0.8732 | 0.7827 | [M:[1.1786, 0.75, 0.8214, 0.8214, 0.75, 0.7857, 0.8214], q:[0.8036, 0.4465], qb:[0.375, 0.8036], phi:[0.3929]] | [M:[[-6], [-14], [6], [6], [-14], [-4], [6]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ | ${}\phi_{1}\tilde{q}_{2}^{2}$ | -3 | 2*t^2.25 + 2*t^2.357 + 3*t^2.464 + t^3.428 + t^3.857 + 3*t^4.5 + 4*t^4.607 + 9*t^4.714 + 7*t^4.821 + 6*t^4.929 + 2*t^5.678 + t^5.786 + t^5.893 - 3*t^6. + t^6.214 + 3*t^6.322 + 4*t^6.75 + 7*t^6.857 + 14*t^6.964 + 15*t^7.071 + 19*t^7.179 + 11*t^7.286 + 7*t^7.393 - t^7.5 + t^7.715 + 3*t^7.928 + 2*t^8.036 + 3*t^8.143 - 7*t^8.25 - 8*t^8.357 - 13*t^8.464 - t^8.572 + 3*t^8.679 + 6*t^8.786 - t^4.179/y - (2*t^6.428)/y - (2*t^6.536)/y - (2*t^6.643)/y + t^7.5/y + (4*t^7.607)/y + (9*t^7.714)/y + (8*t^7.821)/y + (5*t^7.929)/y - t^8.678/y - (2*t^8.786)/y - (4*t^8.893)/y - t^4.179*y - 2*t^6.428*y - 2*t^6.536*y - 2*t^6.643*y + t^7.5*y + 4*t^7.607*y + 9*t^7.714*y + 8*t^7.821*y + 5*t^7.929*y - t^8.678*y - 2*t^8.786*y - 4*t^8.893*y | (2*t^2.25)/g1^14 + (2*t^2.357)/g1^4 + 3*g1^6*t^2.464 + t^3.428/g1^16 + g1^24*t^3.857 + (3*t^4.5)/g1^28 + (4*t^4.607)/g1^18 + (9*t^4.714)/g1^8 + 7*g1^2*t^4.821 + 6*g1^12*t^4.929 + (2*t^5.678)/g1^30 + t^5.786/g1^20 + t^5.893/g1^10 - 3*t^6. + g1^20*t^6.214 + 3*g1^30*t^6.322 + (4*t^6.75)/g1^42 + (7*t^6.857)/g1^32 + (14*t^6.964)/g1^22 + (15*t^7.071)/g1^12 + (19*t^7.179)/g1^2 + 11*g1^8*t^7.286 + 7*g1^18*t^7.393 - g1^28*t^7.5 + g1^48*t^7.715 + (3*t^7.928)/g1^44 + (2*t^8.036)/g1^34 + (3*t^8.143)/g1^24 - (7*t^8.25)/g1^14 - (8*t^8.357)/g1^4 - 13*g1^6*t^8.464 - g1^16*t^8.572 + 3*g1^26*t^8.679 + 6*g1^36*t^8.786 - t^4.179/(g1^2*y) - (2*t^6.428)/(g1^16*y) - (2*t^6.536)/(g1^6*y) - (2*g1^4*t^6.643)/y + t^7.5/(g1^28*y) + (4*t^7.607)/(g1^18*y) + (9*t^7.714)/(g1^8*y) + (8*g1^2*t^7.821)/y + (5*g1^12*t^7.929)/y - t^8.678/(g1^30*y) - (2*t^8.786)/(g1^20*y) - (4*t^8.893)/(g1^10*y) - (t^4.179*y)/g1^2 - (2*t^6.428*y)/g1^16 - (2*t^6.536*y)/g1^6 - 2*g1^4*t^6.643*y + (t^7.5*y)/g1^28 + (4*t^7.607*y)/g1^18 + (9*t^7.714*y)/g1^8 + 8*g1^2*t^7.821*y + 5*g1^12*t^7.929*y - (t^8.678*y)/g1^30 - (2*t^8.786*y)/g1^20 - (4*t^8.893*y)/g1^10 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 1204 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6685 | 0.8477 | 0.7886 | [M:[1.1747, 0.7409, 0.8253, 0.8253, 0.7409, 0.7831], q:[0.8042, 0.4549], qb:[0.3704, 0.8042], phi:[0.3916]] | 2*t^2.223 + 2*t^2.349 + 2*t^2.476 + t^3.397 + t^3.524 + t^3.904 + 3*t^4.445 + 4*t^4.572 + 7*t^4.699 + 5*t^4.825 + 3*t^4.952 + 2*t^5.62 + 3*t^5.747 + 2*t^5.873 - t^6. - t^4.175/y - t^4.175*y | detail |