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 |
|---|---|---|---|---|---|---|---|---|---|
| 1462 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{1}M_{7}$ | 0.7041 | 0.8617 | 0.8171 | [M:[1.0435, 0.8694, 0.913, 1.0, 1.0, 1.087, 0.9565], q:[0.5218, 0.4347], qb:[0.5653, 0.5653], phi:[0.4782]] | [M:[[2, 2], [-6, -6], [-7, -1], [3, -3], [-3, 3], [7, 1], [-2, -2]], q:[[1, 1], [-3, -3]], qb:[[6, 0], [0, 6]], phi:[[-1, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{4}^{2}$, ${ }M_{5}^{2}$ | -3 | t^2.608 + 2*t^2.869 + 2*t^3. + 2*t^3.261 + t^4.043 + t^4.304 + 2*t^4.435 + t^4.565 + 2*t^4.696 + 3*t^4.826 + t^5.217 + 2*t^5.478 + 2*t^5.739 + 4*t^5.869 - 3*t^6. + 2*t^6.131 + 2*t^6.261 - 2*t^6.392 + 3*t^6.522 + t^6.651 + 3*t^6.912 + 2*t^7.043 + t^7.174 + 6*t^7.304 + 2*t^7.435 + 2*t^7.565 + 7*t^7.696 + t^7.825 + 2*t^7.826 + 3*t^8.086 + 4*t^8.088 + 3*t^8.347 + 2*t^8.478 - t^8.608 + 6*t^8.739 - 4*t^8.869 - t^4.435/y - t^7.043/y - t^7.304/y + t^7.565/y + t^7.826/y + (2*t^8.478)/y + (2*t^8.608)/y + t^8.739/y + (6*t^8.869)/y - t^4.435*y - t^7.043*y - t^7.304*y + t^7.565*y + t^7.826*y + 2*t^8.478*y + 2*t^8.608*y + t^8.739*y + 6*t^8.869*y | t^2.608/(g1^6*g2^6) + (2*t^2.869)/(g1^2*g2^2) + (g1^3*t^3.)/g2^3 + (g2^3*t^3.)/g1^3 + g1^7*g2*t^3.261 + g1*g2^7*t^3.261 + t^4.043/(g1^7*g2^7) + t^4.304/(g1^3*g2^3) + (g1^2*t^4.435)/g2^4 + (g2^2*t^4.435)/g1^4 + g1*g2*t^4.565 + g1^6*t^4.696 + g2^6*t^4.696 + (g1^11*t^4.826)/g2 + g1^5*g2^5*t^4.826 + (g2^11*t^4.826)/g1 + t^5.217/(g1^12*g2^12) + (2*t^5.478)/(g1^8*g2^8) + (2*t^5.739)/(g1^4*g2^4) + (2*g1*t^5.869)/g2^5 + (2*g2*t^5.869)/g1^5 - 3*t^6. + (g1^5*t^6.131)/g2 + (g2^5*t^6.131)/g1 + (g1^10*t^6.261)/g2^2 + (g2^10*t^6.261)/g1^2 - g1^9*g2^3*t^6.392 - g1^3*g2^9*t^6.392 + g1^14*g2^2*t^6.522 + g1^8*g2^8*t^6.522 + g1^2*g2^14*t^6.522 + t^6.651/(g1^13*g2^13) + (3*t^6.912)/(g1^9*g2^9) + t^7.043/(g1^4*g2^10) + t^7.043/(g1^10*g2^4) + t^7.174/(g1^5*g2^5) + (3*t^7.304)/g1^6 + (3*t^7.304)/g2^6 + (g1^5*t^7.435)/g2^7 + (g2^5*t^7.435)/g1^7 + (g1^4*t^7.565)/g2^2 + (g2^4*t^7.565)/g1^2 + (3*g1^9*t^7.696)/g2^3 + g1^3*g2^3*t^7.696 + (3*g2^9*t^7.696)/g1^3 + t^7.825/(g1^18*g2^18) + (g1^14*t^7.826)/g2^4 + (g2^14*t^7.826)/g1^4 + (3*t^8.086)/(g1^14*g2^14) + g1^18*t^8.088 + g1^12*g2^6*t^8.088 + g1^6*g2^12*t^8.088 + g2^18*t^8.088 + (3*t^8.347)/(g1^10*g2^10) + t^8.478/(g1^5*g2^11) + t^8.478/(g1^11*g2^5) - t^8.608/(g1^6*g2^6) + (3*t^8.739)/(g1*g2^7) + (3*t^8.739)/(g1^7*g2) + (g1^4*t^8.869)/g2^8 - (6*t^8.869)/(g1^2*g2^2) + (g2^4*t^8.869)/g1^8 - t^4.435/(g1*g2*y) - t^7.043/(g1^7*g2^7*y) - t^7.304/(g1^3*g2^3*y) + (g1*g2*t^7.565)/y + (g1^5*g2^5*t^7.826)/y + (2*t^8.478)/(g1^8*g2^8*y) + t^8.608/(g1^3*g2^9*y) + t^8.608/(g1^9*g2^3*y) + t^8.739/(g1^4*g2^4*y) + (3*g1*t^8.869)/(g2^5*y) + (3*g2*t^8.869)/(g1^5*y) - (t^4.435*y)/(g1*g2) - (t^7.043*y)/(g1^7*g2^7) - (t^7.304*y)/(g1^3*g2^3) + g1*g2*t^7.565*y + g1^5*g2^5*t^7.826*y + (2*t^8.478*y)/(g1^8*g2^8) + (t^8.608*y)/(g1^3*g2^9) + (t^8.608*y)/(g1^9*g2^3) + (t^8.739*y)/(g1^4*g2^4) + (3*g1*t^8.869*y)/g2^5 + (3*g2*t^8.869*y)/g1^5 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 949 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.7004 | 0.8555 | 0.8187 | [M:[1.0368, 0.8895, 0.9263, 1.0, 1.0, 1.0737], q:[0.5184, 0.4448], qb:[0.5552, 0.5552], phi:[0.4816]] | t^2.669 + t^2.89 + 2*t^3. + t^3.11 + 2*t^3.221 + t^4.113 + t^4.334 + 2*t^4.445 + t^4.555 + 2*t^4.666 + 3*t^4.776 + t^5.337 + t^5.558 + t^5.779 + 2*t^5.89 - 2*t^6. - t^4.445/y - t^4.445*y | detail |