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 |
|---|---|---|---|---|---|---|---|---|---|
| 58743 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ + ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}M_{8}$ | 0.7057 | 0.8665 | 0.8144 | [M:[1.0, 0.9827, 1.0173, 1.1111, 0.7951, 0.7605, 0.7778, 1.2049], q:[0.3889, 0.6111], qb:[0.6284, 0.5938], phi:[0.4444]] | [M:[[0], [1], [-1], [0], [-1], [1], [0], [1]], q:[[0], [0]], qb:[[-1], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{8}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{1}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{2}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{1}M_{2}$, ${ }M_{7}M_{8}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -1 | t^2.282 + t^2.333 + t^2.948 + t^3. + t^3.052 + t^3.333 + t^3.615 + t^3.667 + t^4.282 + t^4.333 + t^4.385 + t^4.563 + t^4.615 + t^4.667 + t^4.896 + t^4.948 + 2*t^5. + t^5.052 + t^5.104 + t^5.23 + t^5.282 + t^5.333 + t^5.615 + t^5.667 + t^5.896 + t^5.948 - t^6. - t^6.052 + t^6.282 + t^6.333 + t^6.385 + 2*t^6.563 + 2*t^6.615 + 2*t^6.667 + t^6.845 + t^6.896 + 2*t^6.948 + t^7. + t^7.178 + 3*t^7.23 + 3*t^7.282 + 3*t^7.333 + t^7.385 + t^7.437 + t^7.511 + t^7.563 + t^7.615 + t^7.845 + 3*t^7.896 + 4*t^7.948 + 3*t^8. + 2*t^8.052 + t^8.104 + t^8.155 + t^8.178 + t^8.23 - 2*t^8.282 - 3*t^8.333 - 2*t^8.385 + t^8.511 + 3*t^8.563 + 3*t^8.615 + 3*t^8.667 + t^8.718 + t^8.77 + 2*t^8.845 + t^8.896 - 2*t^8.948 - t^4.333/y - t^6.615/y - t^6.667/y + t^7.615/y + t^8./y + t^8.052/y + t^8.23/y + (2*t^8.282)/y + (2*t^8.333)/y + t^8.385/y + t^8.615/y + t^8.667/y + (2*t^8.948)/y - t^4.333*y - t^6.615*y - t^6.667*y + t^7.615*y + t^8.*y + t^8.052*y + t^8.23*y + 2*t^8.282*y + 2*t^8.333*y + t^8.385*y + t^8.615*y + t^8.667*y + 2*t^8.948*y | g1*t^2.282 + t^2.333 + g1*t^2.948 + t^3. + t^3.052/g1 + t^3.333 + g1*t^3.615 + t^3.667 + g1*t^4.282 + t^4.333 + t^4.385/g1 + g1^2*t^4.563 + g1*t^4.615 + t^4.667 + g1^2*t^4.896 + g1*t^4.948 + 2*t^5. + t^5.052/g1 + t^5.104/g1^2 + g1^2*t^5.23 + g1*t^5.282 + t^5.333 + g1*t^5.615 + t^5.667 + g1^2*t^5.896 + g1*t^5.948 - t^6. - t^6.052/g1 + g1*t^6.282 + t^6.333 + t^6.385/g1 + 2*g1^2*t^6.563 + 2*g1*t^6.615 + 2*t^6.667 + g1^3*t^6.845 + g1^2*t^6.896 + 2*g1*t^6.948 + t^7. + g1^3*t^7.178 + 3*g1^2*t^7.23 + 3*g1*t^7.282 + 3*t^7.333 + t^7.385/g1 + t^7.437/g1^2 + g1^3*t^7.511 + g1^2*t^7.563 + g1*t^7.615 + g1^3*t^7.845 + 3*g1^2*t^7.896 + 4*g1*t^7.948 + 3*t^8. + (2*t^8.052)/g1 + t^8.104/g1^2 + t^8.155/g1^3 + g1^3*t^8.178 + g1^2*t^8.23 - 2*g1*t^8.282 - 3*t^8.333 - (2*t^8.385)/g1 + g1^3*t^8.511 + 3*g1^2*t^8.563 + 3*g1*t^8.615 + 3*t^8.667 + t^8.718/g1 + t^8.77/g1^2 + 2*g1^3*t^8.845 + g1^2*t^8.896 - 2*g1*t^8.948 - t^4.333/y - (g1*t^6.615)/y - t^6.667/y + (g1*t^7.615)/y + t^8./y + t^8.052/(g1*y) + (g1^2*t^8.23)/y + (2*g1*t^8.282)/y + (2*t^8.333)/y + t^8.385/(g1*y) + (g1*t^8.615)/y + t^8.667/y + (2*g1*t^8.948)/y - t^4.333*y - g1*t^6.615*y - t^6.667*y + g1*t^7.615*y + t^8.*y + (t^8.052*y)/g1 + g1^2*t^8.23*y + 2*g1*t^8.282*y + 2*t^8.333*y + (t^8.385*y)/g1 + g1*t^8.615*y + t^8.667*y + 2*g1*t^8.948*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 56896 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ + ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ | 0.723 | 0.8966 | 0.8064 | [M:[1.0, 1.0, 1.0, 1.1111, 0.7778, 0.7778, 0.7778], q:[0.3889, 0.6111], qb:[0.6111, 0.6111], phi:[0.4444]] | 3*t^2.333 + 3*t^3. + t^3.333 + t^3.667 + 3*t^4.333 + 6*t^4.667 + 6*t^5. + 6*t^5.333 + 3*t^5.667 - t^6. - t^4.333/y - t^4.333*y | detail | {a: 937/1296, c: 581/648, M1: 1, M2: 1, M3: 1, M4: 10/9, M5: 7/9, M6: 7/9, M7: 7/9, q1: 7/18, q2: 11/18, qb1: 11/18, qb2: 11/18, phi1: 4/9} |