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 |
|---|---|---|---|---|---|---|---|---|---|
| 56699 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{4}M_{6}$ + ${ }M_{3}M_{7}$ | 0.7051 | 0.8701 | 0.8103 | [M:[0.9231, 0.8719, 1.0256, 1.0769, 1.0, 0.9231, 0.9744], q:[0.5769, 0.5], qb:[0.5512, 0.4231], phi:[0.4872]] | [M:[[6], [10], [-2], [-6], [0], [6], [2]], q:[[-6], [0]], qb:[[-4], [6]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{6}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$ | ${}$ | -3 | t^2.616 + 2*t^2.769 + 2*t^2.923 + t^3. + t^3.154 + t^4. + t^4.231 + t^4.385 + 2*t^4.462 + t^4.615 + t^4.692 + t^4.769 + t^4.846 + t^4.923 + t^5.231 + 2*t^5.385 + 4*t^5.539 + 4*t^5.693 + t^5.769 + 2*t^5.846 + 3*t^5.923 - 3*t^6. + t^6.077 - t^6.154 - 2*t^6.231 + t^6.307 - t^6.384 - t^6.461 + t^6.616 + 2*t^6.77 + t^6.847 + 2*t^6.924 + 3*t^7. + 4*t^7.154 + 3*t^7.231 + t^7.308 + 6*t^7.385 + 2*t^7.538 + 3*t^7.615 + t^7.692 + 2*t^7.769 + t^7.847 - t^8. + 3*t^8.001 + 4*t^8.154 + t^8.231 + 6*t^8.308 + 8*t^8.462 + 2*t^8.616 + 5*t^8.693 - 5*t^8.769 + 4*t^8.846 - 6*t^8.923 - t^4.462/y - t^7.077/y - t^7.231/y - t^7.385/y + t^7.538/y + t^7.692/y + t^7.846/y + (2*t^8.385)/y + (3*t^8.539)/y + t^8.616/y + (4*t^8.693)/y + (3*t^8.769)/y + t^8.846/y + (4*t^8.923)/y - t^4.462*y - t^7.077*y - t^7.231*y - t^7.385*y + t^7.538*y + t^7.692*y + t^7.846*y + 2*t^8.385*y + 3*t^8.539*y + t^8.616*y + 4*t^8.693*y + 3*t^8.769*y + t^8.846*y + 4*t^8.923*y | g1^10*t^2.616 + 2*g1^6*t^2.769 + 2*g1^2*t^2.923 + t^3. + t^3.154/g1^4 + g1^13*t^4. + g1^7*t^4.231 + g1^3*t^4.385 + 2*g1*t^4.462 + t^4.615/g1^3 + t^4.692/g1^5 + t^4.769/g1^7 + t^4.846/g1^9 + t^4.923/g1^11 + g1^20*t^5.231 + 2*g1^16*t^5.385 + 4*g1^12*t^5.539 + 4*g1^8*t^5.693 + g1^6*t^5.769 + 2*g1^4*t^5.846 + 3*g1^2*t^5.923 - 3*t^6. + t^6.077/g1^2 - t^6.154/g1^4 - (2*t^6.231)/g1^6 + t^6.307/g1^8 - t^6.384/g1^10 - t^6.461/g1^12 + g1^23*t^6.616 + 2*g1^19*t^6.77 + g1^17*t^6.847 + 2*g1^15*t^6.924 + 3*g1^13*t^7. + 4*g1^9*t^7.154 + 3*g1^7*t^7.231 + g1^5*t^7.308 + 6*g1^3*t^7.385 + (2*t^7.538)/g1 + (3*t^7.615)/g1^3 + t^7.692/g1^5 + (2*t^7.769)/g1^7 + g1^30*t^7.847 - t^8./g1^13 + 3*g1^26*t^8.001 + 4*g1^22*t^8.154 + g1^20*t^8.231 + 6*g1^18*t^8.308 + 8*g1^14*t^8.462 + 2*g1^10*t^8.616 + 5*g1^8*t^8.693 - 5*g1^6*t^8.769 + 4*g1^4*t^8.846 - 6*g1^2*t^8.923 - (g1*t^4.462)/y - (g1^11*t^7.077)/y - (g1^7*t^7.231)/y - (g1^3*t^7.385)/y + t^7.538/(g1*y) + t^7.692/(g1^5*y) + t^7.846/(g1^9*y) + (2*g1^16*t^8.385)/y + (3*g1^12*t^8.539)/y + (g1^10*t^8.616)/y + (4*g1^8*t^8.693)/y + (3*g1^6*t^8.769)/y + (g1^4*t^8.846)/y + (4*g1^2*t^8.923)/y - g1*t^4.462*y - g1^11*t^7.077*y - g1^7*t^7.231*y - g1^3*t^7.385*y + (t^7.538*y)/g1 + (t^7.692*y)/g1^5 + (t^7.846*y)/g1^9 + 2*g1^16*t^8.385*y + 3*g1^12*t^8.539*y + g1^10*t^8.616*y + 4*g1^8*t^8.693*y + 3*g1^6*t^8.769*y + g1^4*t^8.846*y + 4*g1^2*t^8.923*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 |
|---|---|---|---|---|---|---|---|---|---|
| 54934 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{4}M_{6}$ | 0.7028 | 0.8656 | 0.8119 | [M:[0.9296, 0.8826, 1.0235, 1.0704, 1.0, 0.9296], q:[0.5704, 0.5], qb:[0.5469, 0.4296], phi:[0.4883]] | t^2.648 + 2*t^2.789 + t^2.93 + t^3. + t^3.07 + t^3.141 + t^4.042 + t^4.254 + t^4.394 + 2*t^4.465 + t^4.606 + t^4.676 + t^4.746 + t^4.817 + t^4.887 + t^5.296 + 2*t^5.437 + 3*t^5.577 + 3*t^5.718 + t^5.789 + 2*t^5.859 + 2*t^5.93 - 2*t^6. - t^4.465/y - t^4.465*y | detail |