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 |
|---|---|---|---|---|---|---|---|---|---|
| 1225 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}q_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{2}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6806 | 0.8472 | 0.8033 | [M:[1.0, 1.1667, 0.9444, 0.8333, 0.8333, 0.7778], q:[0.7778, 0.3889], qb:[0.6111, 0.4444], phi:[0.4444]] | [M:[[0], [-3], [-11], [3], [3], [10]], q:[[1], [-4]], qb:[[4], [7]], phi:[[-2]]] | 1 | {a: 49/72, c: 61/72, M1: 1, M2: 7/6, M3: 17/18, M4: 5/6, M5: 5/6, M6: 7/9, q1: 7/9, q2: 7/18, qb1: 11/18, qb2: 4/9, phi1: 4/9} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{3}^{2}$, ${ }M_{1}\phi_{1}^{2}$ | ${}M_{6}q_{1}\tilde{q}_{2}$ | -1 | t^2.333 + 2*t^2.5 + t^2.667 + t^2.833 + t^3. + t^3.667 + t^3.833 + t^4. + t^4.167 + t^4.333 + t^4.5 + t^4.667 + 2*t^4.833 + 5*t^5. + 3*t^5.167 + 3*t^5.333 + 2*t^5.5 + 2*t^5.667 - t^6. + t^6.167 + 3*t^6.333 + 3*t^6.5 + 3*t^6.667 + 3*t^6.833 + 3*t^7. + 2*t^7.167 + 4*t^7.333 + 8*t^7.5 + 7*t^7.667 + 5*t^7.833 + 6*t^8. + 3*t^8.167 - 2*t^8.5 + t^8.667 + 2*t^8.833 - t^4.333/y - t^6.667/y - t^6.833/y - t^7./y - t^7.167/y + t^7.5/y + t^7.667/y + (3*t^7.833)/y + (3*t^8.)/y + (3*t^8.167)/y + (3*t^8.333)/y + (3*t^8.5)/y + t^8.667/y + t^8.833/y - t^4.333*y - t^6.667*y - t^6.833*y - t^7.*y - t^7.167*y + t^7.5*y + t^7.667*y + 3*t^7.833*y + 3*t^8.*y + 3*t^8.167*y + 3*t^8.333*y + 3*t^8.5*y + t^8.667*y + t^8.833*y | g1^10*t^2.333 + 2*g1^3*t^2.5 + t^2.667/g1^4 + t^2.833/g1^11 + t^3. + g1^8*t^3.667 + g1*t^3.833 + g1^12*t^4. + g1^5*t^4.167 + t^4.333/g1^2 + g1^9*t^4.5 + g1^20*t^4.667 + 2*g1^13*t^4.833 + 5*g1^6*t^5. + (3*t^5.167)/g1 + (2*t^5.333)/g1^8 + g1^10*t^5.333 + t^5.5/g1^15 + g1^3*t^5.5 + t^5.667/g1^22 + t^5.667/g1^4 - 2*t^6. + g1^18*t^6. - t^6.167/g1^7 + 2*g1^11*t^6.167 + 2*g1^4*t^6.333 + g1^22*t^6.333 + 3*g1^15*t^6.5 + 3*g1^8*t^6.667 + 2*g1*t^6.833 + g1^19*t^6.833 + 2*g1^12*t^7. + g1^30*t^7. + 2*g1^23*t^7.167 - t^7.333/g1^2 + 5*g1^16*t^7.333 + 8*g1^9*t^7.5 + 5*g1^2*t^7.667 + 2*g1^20*t^7.667 + (3*t^7.833)/g1^5 + 2*g1^13*t^7.833 + (3*t^8.)/g1^12 + 2*g1^6*t^8. + g1^24*t^8. + (2*t^8.167)/g1^19 + g1^17*t^8.167 + t^8.333/g1^26 - 2*g1^10*t^8.333 + g1^28*t^8.333 + t^8.5/g1^33 - 6*g1^3*t^8.5 + 3*g1^21*t^8.5 - (4*t^8.667)/g1^4 + 4*g1^14*t^8.667 + g1^32*t^8.667 - (3*t^8.833)/g1^11 + 2*g1^7*t^8.833 + 3*g1^25*t^8.833 - t^4.333/(g1^2*y) - (g1^8*t^6.667)/y - (g1*t^6.833)/y - t^7./(g1^6*y) - t^7.167/(g1^13*y) + (g1^9*t^7.5)/y + (g1^2*t^7.667)/y + t^7.833/(g1^5*y) + (2*g1^13*t^7.833)/y + t^8./(g1^12*y) + (2*g1^6*t^8.)/y + (3*t^8.167)/(g1*y) + (2*t^8.333)/(g1^8*y) + (g1^10*t^8.333)/y + t^8.5/(g1^15*y) + (2*g1^3*t^8.5)/y + t^8.667/(g1^4*y) + t^8.833/(g1^11*y) - (t^4.333*y)/g1^2 - g1^8*t^6.667*y - g1*t^6.833*y - (t^7.*y)/g1^6 - (t^7.167*y)/g1^13 + g1^9*t^7.5*y + g1^2*t^7.667*y + (t^7.833*y)/g1^5 + 2*g1^13*t^7.833*y + (t^8.*y)/g1^12 + 2*g1^6*t^8.*y + (3*t^8.167*y)/g1 + (2*t^8.333*y)/g1^8 + g1^10*t^8.333*y + (t^8.5*y)/g1^15 + 2*g1^3*t^8.5*y + (t^8.667*y)/g1^4 + (t^8.833*y)/g1^11 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 745 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}q_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{2}M_{5}$ | 0.6636 | 0.816 | 0.8132 | [M:[1.0, 1.1577, 0.9114, 0.8423, 0.8423], q:[0.7808, 0.3769], qb:[0.6231, 0.4655], phi:[0.4384]] | 2*t^2.527 + t^2.631 + t^2.734 + t^3. + t^3.577 + t^3.739 + t^3.842 + t^4.108 + t^4.212 + t^4.315 + t^4.581 + 4*t^5.054 + 2*t^5.158 + 2*t^5.261 + t^5.365 + t^5.468 + t^5.527 + t^5.631 - 2*t^6. - t^4.315/y - t^4.315*y | detail |